Optical Image Capturing System

ABSTRACT

A six-piece optical lens for capturing image and a six-piece optical module for capturing image are provided. In order from an object side to an image side, the optical lens along the optical axis includes a first lens with refractive power, a second lens with refractive power, a third lens with refractive power, a fourth lens with refractive power, a fifth lens with refractive power and a sixth lens with refractive power. At least one of the image-side surface and object-side surface of each of the six lens elements is aspheric. The optical lens can increase aperture value and improve the imagining quality for use in compact cameras.

CROSS-REFERENCE TO RELATED APPLICATION

This application claims the benefit of Taiwan Patent Application No.104140210, filed on Dec. 1, 2015, in the Taiwan Intellectual PropertyOffice, the disclosure of which is incorporated herein in its entiretyby reference.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present disclosure relates to an optical image capturing system, andmore particularly to a compact optical image capturing system which canbe applied to electronic products.

2. Description of the Related Art

In recent years, with the rise of portable electronic devices havingcamera functionalities, the demand for an optical image capturing systemis raised gradually. The image sensing device of ordinary photographingcamera is commonly selected from charge coupled device (CCD) orcomplementary metal-oxide semiconductor sensor (CMOS Sensor). Inaddition, as advanced semiconductor manufacturing technology enables theminimization of pixel size of the image sensing device, the developmentof the optical image capturing system directs towards the field of highpixels. Therefore, the requirement for high imaging quality is rapidlyraised.

The traditional optical image capturing system of a portable electronicdevice comes with different designs, including a four-lens or afifth-lens design. However, the requirement for the higher pixels andthe requirement for a large aperture of an end user, likefunctionalities of micro filming and night view have been raised. Theoptical image capturing system in prior arts cannot meet the requirementof the higher order camera lens module.

Therefore, how to effectively increase quantity of incoming light of theoptical lenses, and further improves imaging quality for the imageformation, becomes a quite important issue.

SUMMARY OF THE INVENTION

The aspect of embodiment of the present disclosure directs to an opticalimage capturing system and an optical image capturing lens which usecombination of refractive powers, convex and concave surfaces ofsix-piece optical lenses (the convex or concave surface in thedisclosure denotes the change of geometrical shape of an object-sidesurface or an image-side surface of each lens with different height froman optical axis) to increase the quantity of incoming light of theoptical image capturing system, and to improve imaging quality for imageformation, so as to be applied to minimized electronic products.

The term and its definition to the lens element parameter in theembodiment of the present invention are shown as below for furtherreference.

The Lens Element Parameter Related to a Length or a Height in the LensElement

A maximum height for image formation of the optical image capturingsystem is denoted by HOI. A height of the optical image capturing systemis denoted by HOS. A distance from the object-side surface of the firstlens element to the image-side surface of the sixth lens element isdenoted by InTL. A distance from an aperture stop (aperture) to an imageplane is denoted by InS. A distance from the first lens element to thesecond lens element is denoted by In12 (instance). A central thicknessof the first lens element of the optical image capturing system on theoptical axis is denoted by TP1 (instance).

The Lens Element Parameter Related to a Material in the Lens Element

An Abbe number of the first lens element in the optical image capturingsystem is denoted by NA1 (instance). A refractive index of the firstlens element is denoted by Nd1 (instance).

The Lens Element Parameter Related to a View Angle in the Lens Element

A view angle is denoted by AF. Half of the view angle is denoted by HAF.A major light angle is denoted by MRA.

The Lens Element Parameter Related to Exit/Entrance Pupil in the LensElement

An entrance pupil diameter of the optical image capturing system isdenoted by HEP. An entrance pupil diameter of the optical imagecapturing system is denoted by HEP. A maximum effective half diameterposition of any surface of single lens element means the vertical heightbetween the effective half diameter (EHD) and the optical axis where theincident light of the maximum view angle of the system passes throughthe farthest edge of the entrance pupil on the EHD of the surface of thelens element. For example, the maximum effective half diameter positionof the object-side surface of the first lens element is denoted asEHD11. The maximum effective half diameter position of the image-side ofthe first lens element is denoted as EHD12. The maximum effective halfdiameter position of the object-side surface of the second lens elementis denoted as EHD21. The maximum half effective half diameter positionof the image-side surface of the second lens element is denoted asEHD22. The maximum effective half diameter position of any surfaces ofthe remaining lens elements of the optical image capturing system can bereferred as mentioned above.

The Lens Element Parameter Related to an Arc Length of the Lens ElementShape and an Outline of Surface

A length of outline curve of the maximum effective half diameterposition of any surface of a single lens element refers to a length ofoutline curve from an axial point on the surface of the lens element tothe maximum effective half diameter position of the surface along anoutline of the surface of the lens element and is denoted as ARS. Forexample, the length of outline curve of the maximum effective halfdiameter position of the object-side surface of the first lens elementis denoted as ARS11. The length of outline curve of the maximumeffective half diameter position of the image-side surface of the firstlens element is denoted as ARS12. The length of outline curve of themaximum effective half diameter position of the object-side surface ofthe second lens element is denoted as ARS21. The length of outline curveof the maximum effective half diameter position of the image-sidesurface of the second lens element is denoted as ARS22. The lengths ofoutline curve of the maximum effective half diameter position of anysurface of the other lens elements in the optical image capturing systemare denoted in the similar way.

A length of outline curve of a half of an entrance pupil diameter (HEP)of any surface of a signal lens element refers to a length of outlinecurve of the half of the entrance pupil diameter (HEP) from an axialpoint on the surface of the lens element to a coordinate point ofvertical height with a distance of the half of the entrance pupildiameter from the optical axis on the surface along the outline of thesurface of the lens element and is denoted as ARE. For example, thelength of the outline curve of the half of the entrance pupil diameter(HEP) of the object-side surface of the first lens element is denoted asARE11. The length of the outline curve of the half of the entrance pupildiameter (HEP) of the image-side surface of the first lens element isdenoted as ARE12. The length of the outline curve of the half of theentrance pupil diameter (HEP) of the object-side surface of the secondlens element is denoted as ARE21. The length of the outline curve of thehalf of the entrance pupil diameter (HEP) of the image-side surface ofthe second lens element is denoted as ARS22. The lengths of outlinecurves of the half of the entrance pupil diameters (HEP) of any surfaceof the other lens elements in the optical image capturing system aredenoted in the similar way.

The Lens Element Parameter Related to a Depth of the Lens Element Shape

A horizontal distance in parallel with an optical axis from a maximumeffective half diameter position to an axial point on the object-sidesurface of the sixth lens element is denoted by InRS61 (a depth of themaximum effective half diameter). A horizontal distance in parallel withan optical axis from a maximum effective half diameter position to anaxial point on the image-side surface of the sixth lens element isdenoted by InRS62 (the depth of the maximum effective half diameter).The depths of the maximum effective half diameters (sinkage values) ofobject surfaces and image surfaces of other lens elements are denoted inthe similar way.

The Lens Element Parameter Related to the Lens Element Shape

A critical point C is a tangent point on a surface of a specific lenselement, and the tangent point is tangent to a plane perpendicular tothe optical axis and the tangent point cannot be a crossover point onthe optical axis. To follow the past, a distance perpendicular to theoptical axis between a critical point CM on the object-side surface ofthe fifth lens element and the optical axis is HVT51 (instance). Adistance perpendicular to the optical axis between a critical point C52on the image-side surface of the fifth lens element and the optical axisis HVT52 (instance). A distance perpendicular to the optical axisbetween a critical point C61 on the object-side surface of the sixthlens element and the optical axis is HVT61 (instance). A distanceperpendicular to the optical axis between a critical point C62 on theimage-side surface of the sixth lens element and the optical axis isHVT62 (instance). Distances perpendicular to the optical axis betweencritical points on the object-side surfaces or the image-side surfacesof other lens elements and the optical axis are denoted in the similarway described above.

The object-side surface of the sixth lens element has one inflectionpoint IF611 which is nearest to the optical axis, and the sinkage valueof the inflection point IF611 is denoted by SGI611. SGI611 is ahorizontal shift distance in parallel with the optical axis from anaxial point on the object-side surface of the sixth lens element to theinflection point which is nearest to the optical axis on the object-sidesurface of the sixth lens element. A distance perpendicular to theoptical axis between the inflection point IF611 and the optical axis isHIF611 (instance). The image-side surface of the sixth lens element hasone inflection point IF621 which is nearest to the optical axis and thesinkage value of the inflection point IF621 is denoted by SGI621(instance). SGI621 is a horizontal shift distance in parallel with theoptical axis from an axial point on the image-side surface of the sixthlens element to the inflection point which is nearest to the opticalaxis on the image-side surface of the sixth lens element. A distanceperpendicular to the optical axis between the inflection point IF621 andthe optical axis is HIF621 (instance).

The object-side surface of the sixth lens element has one inflectionpoint IF612 which is the second nearest to the optical axis and thesinkage value of the inflection point IF612 is denoted by SGI612(instance). SGI612 is a horizontal shift distance in parallel with theoptical axis from an axial point on the object-side surface of the sixthlens element to the inflection point which is the second nearest to theoptical axis on the object-side surface of the sixth lens element. Adistance perpendicular to the optical axis between the inflection pointIF612 and the optical axis is HIF612 (instance). The image-side surfaceof the sixth lens element has one inflection point IF622 which is thesecond nearest to the optical axis and the sinkage value of theinflection point IF622 is denoted by SGI622 (instance). SGI622 is ahorizontal shift distance in parallel with the optical axis from anaxial point on the image-side surface of the sixth lens element to theinflection point which is the second nearest to the optical axis on theimage-side surface of the sixth lens element. A distance perpendicularto the optical axis between the inflection point IF622 and the opticalaxis is HIF622 (instance).

The object-side surface of the sixth lens element has one inflectionpoint IF613 which is the third nearest to the optical axis and thesinkage value of the inflection point IF613 is denoted by SGI613(instance). SGI613 is a horizontal shift distance in parallel with theoptical axis from an axial point on the object-side surface of the sixthlens element to the inflection point which is the third nearest to theoptical axis on the object-side surface of the sixth lens element. Adistance perpendicular to the optical axis between the inflection pointIF613 and the optical axis is HIF613 (instance). The image-side surfaceof the sixth lens element has one inflection point IF623 which is thethird nearest to the optical axis and the sinkage value of theinflection point IF623 is denoted by SGI623 (instance). SGI623 is ahorizontal shift distance in parallel with the optical axis from anaxial point on the image-side surface of the sixth lens element to theinflection point which is the third nearest to the optical axis on theimage-side surface of the sixth lens element. A distance perpendicularto the optical axis between the inflection point IF623 and the opticalaxis is HIF623 (instance).

The object-side surface of the sixth lens element has one inflectionpoint IF614 which is the fourth nearest to the optical axis and thesinkage value of the inflection point IF614 is denoted by SGI614(instance). SGI614 is a horizontal shift distance in parallel with theoptical axis from an axial point on the object-side surface of the sixthlens element to the inflection point which is the fourth nearest to theoptical axis on the object-side surface of the sixth lens element. Adistance perpendicular to the optical axis between the inflection pointIF614 and the optical axis is HIF614 (instance). The image-side surfaceof the sixth lens element has one inflection point IF624 which is thefourth nearest to the optical axis and the sinkage value of theinflection point IF624 is denoted by SGI624 (instance). SGI624 is ahorizontal shift distance in parallel with the optical axis from anaxial point on the image-side surface of the sixth lens element to theinflection point which is the fourth nearest to the optical axis on theimage-side surface of the sixth lens element. A distance perpendicularto the optical axis between the inflection point IF624 and the opticalaxis is HIF624 (instance).

The inflection points on the object-side surfaces or the image-sidesurfaces of the other lens elements and the distances perpendicular tothe optical axis thereof or the sinkage values thereof are denoted inthe similar way described above.

The Lens Element Parameter Related to an Aberration

Optical distortion for image formation in the optical image capturingsystem is denoted by ODT. TV distortion for image formation in theoptical image capturing system is denoted by TDT. Further, the range ofthe aberration offset for the view of image formation may be limited to50%-100%. An offset of the spherical aberration is denoted by DFS. Anoffset of the coma aberration is denoted by DFC.

The lateral aberration of the stop is denoted as STA to assess thefunction of the specific optical image capturing system. The tangentialfan or sagittal fan may be applied to calculate the STA of any viewfields, and in particular, to calculate the STA of the max referencewavelength (e.g. 650 nm) and the minima reference wavelength (e.g. 470nm) for serve as the standard of the optimal function. Theaforementioned direction of the tangential fan can be further defined asthe positive (overhead-light) and negative (lower-light) directions. Themax operation wavelength, which passes through the STA, is defined asthe image position of the specific view field, and the distancedifference of two positions of image position of the view field betweenthe max operation wavelength and the reference primary wavelength (e.g.wavelength of 555 nm), and the minimum operation wavelength, whichpasses through the STA, is defined as the image position of the specificview field, and STA of the max operation wavelength is defined as thedistance between the image position of the specific view field of maxoperation wavelength and the image position of the specific view fieldof the reference primary wavelength (e.g. wavelength of 555 nm), and STAof the minimum operation wavelength is defined as the distance betweenthe image position of the specific view field of the minimum operationwavelength and the image position of the specific view field of thereference primary wavelength (e.g. wavelength of 555 nm) are assessedthe function of the specific optical image capturing system to beoptimal. Both STA of the max operation wavelength and STA of the minimumoperation wavelength on the image position of vertical height with adistance from the optical axis to 70% HOI (i.e. 0.7 HOI), which aresmaller than 100,a m, are served as the sample. The numerical, which aresmaller than 80,a m, are also served as the sample.

A maximum height for image formation on the image plane perpendicular tothe optical axis in the optical image capturing system is denoted byHOI. A lateral aberration of the longest operation wavelength of avisible light of a positive direction tangential fan of the opticalimage capturing system passing through an edge of the entrance pupil andincident on the image plane by 0.7 HOI is denoted as PLTA. A lateralaberration of the shortest operation wavelength of a visible light ofthe positive direction tangential fan of the optical image capturingsystem passing through the edge of the entrance pupil and incident onthe image plane by 0.7 HOI is denoted as PSTA. A lateral aberration ofthe longest operation wavelength of a visible light of a negativedirection tangential fan of the optical image capturing system passingthrough the edge of the entrance pupil and incident on the image planeby 0.7 HOI is denoted as NLTA. A lateral aberration of the shortestoperation wavelength of a visible light of a negative directiontangential fan of the optical image capturing system passing through theedge of the entrance pupil and incident on the image plane by 0.7 HOI isdenoted as NSTA. A lateral aberration of the longest operationwavelength of a visible light of a sagittal fan of the optical imagecapturing system passing through the edge of the entrance pupil andincident on the image plane by 0.7 HOI is denoted as SLTA. A lateralaberration of the shortest operation wavelength of a visible light ofthe sagittal fan of the optical image capturing system passing throughthe edge of the entrance pupil and incident on the image plane by 0.7HOI is denoted as SSTA.

The disclosure provides an optical image capturing system, anobject-side surface or an image-side surface of the sixth lens elementmay have inflection points, such that the angle of incidence from eachview field to the sixth lens element can be adjusted effectively and theoptical distortion and the TV distortion can be corrected as well.Besides, the surfaces of the sixth lens element may have a betteroptical path adjusting ability to acquire better imaging quality.

The disclosure provides an optical image capturing system, in order froman object side to an image side, including a first, second, third,fourth, fifth, sixth lens elements and an image plane. The first lenselement has refractive power. An object-side surface and an image-sidesurface of the sixth lens element are aspheric. Focal lengths of thefirst through sixth lens elements are f1, f2, f3, f4, f5 and f6respectively. A focal length of the optical image capturing system is fAn entrance pupil diameter of the optical image capturing system is HEP.A distance on an optical axis from an object-side surface of the firstlens element to the image plane is HOS. A distance on the optical axisfrom the object-side surface of the first lens element to the image-sidesurface of the sixth lens element is InTL. A half of a maximum viewangle of the optical image capturing system is HAF. A length of outlinecurve from an axial point on any surface of any one of the six lenselements to a coordinate point of vertical height with a distance of ahalf of the entrance pupil diameter from the optical axis on the surfacealong an outline of the surface is denoted as ARE. The followingrelations are satisfied: 1.0≦f/HEP≦10.0, 0 deg<HAF≦150 deg and0.9≦2(ARE/HEP)≦1.5.

The disclosure provides another optical image capturing system, in orderfrom an object side to an image side, including a first, second, third,fourth, fifth, six lens elements and an image plane. The first lenselement has refractive power. The second lens element has refractivepower. The third lens element has refractive power. The fourth lenselement has refractive power. The fifth lens element has refractivepower. The sixth lens element has refractive power. At least one lenselement among the first through the sixth lens elements has at least oneinflection point on at least one surface thereof, and at least one lenselement among the first through third lens elements has positiverefractive power, and at least one lens element among the fourth throughsixth lens elements has positive refractive power. Focal lengths of thefirst through sixth lens elements are f1, f2, f3, f4, f5 and f6,respectively. A focal length of the optical image capturing system is f.An entrance pupil diameter of the optical image capturing system is HEP.A distance on an optical axis from an object-side surface of the firstlens element to the image plane is HOS. A distance on the optical axisfrom the object-side surface of the first lens element to the image-sidesurface of the sixth lens element is InTL A half of a maximum view angleof the optical image capturing system is HAF. A length of outline curvefrom an axial point on any surface of any one of the six lens elementsto a coordinate point of vertical height with a distance of a half ofthe entrance pupil diameter from the optical axis on the surface alongan outline of the surface is denoted as ARE. The following relations aresatisfied: 1.0≦f/HEP≦10.0, 0 deg<HAF≦150 deg and 0.9≦2(ARE/HEP)≦1.5.

The disclosure provides another optical image capturing system, in orderfrom an object side to an image side, including a first, second, third,fourth, fifth, sixth lens elements and an image plane. Wherein, theoptical image capturing system consists of the six lens elements withrefractive power. The first lens element has positive refractive power.The second lens element has refractive power. The third lens element hasrefractive power. The fourth lens element has refractive power. Thefifth lens element has refractive power. The sixth lens element hasrefractive power. At least one lens element among the second through thesixth lens elements has positive refractive power. At least two lenselements among the first through the sixth lens elements respectivelyhave at least one inflection point on at least one surface thereof.Focal lengths of the first through sixth lens elements are f1, f2, f3,f4, f5 and f6 respectively. A focal length of the optical imagecapturing system is f An entrance pupil diameter of the optical imagecapturing system is HEP. A distance on an optical axis from anobject-side surface of the first lens element to the image plane is HOS.A distance on the optical axis from the object-side surface of the firstlens element to the image-side surface of the sixth lens element is InTLA half of a maximum view angle of the optical image capturing system isHAF. A length of outline curve from an axial point on any surface of anyone of the six lens elements to a coordinate point of vertical heightwith a distance of a half of the entrance pupil diameter from theoptical axis on the surface along an outline of the surface is denotedas ARE. The following relations are satisfied: 1≦f/HEP 3.5, 0deg<HAF≦150 deg and 0.9≦2(ARE/HEP)≦1.5.

The length of the outline curve of any surface of a signal lens elementin the maximum effective half diameter position affects the functions ofthe surface aberration correction and the optical path difference ineach view field. The longer outline curve may lead to a better functionof aberration correction, but the difficulty of the production maybecome inevitable. Hence, the length of the outline curve of the maximumeffective half diameter position of any surface of a signal lens element(ARS) has to be controlled, and especially, the ratio relations (ARS/TP)between the length of the outline curve of the maximum effective halfdiameter position of the surface (ARS) and the thickness of the lenselement to which the surface belongs on the optical axis (TP) has to becontrolled. For example, the length of the outline curve of the maximumeffective half diameter position of the object-side surface of the firstlens element is denoted as ARS11, and the thickness of the first lenselement on the optical axis is TP1, and the ratio between both of themis ARS11/TP1. The length of the outline curve of the maximum effectivehalf diameter position of the image-side surface of the first lenselement is denoted as ARS12, and the ratio between ARS12 and TP1 isARS12/TP1. The length of the outline curve of the maximum effective halfdiameter position of the object-side surface of the second lens elementis denoted as ARS21, and the thickness of the second lens element on theoptical axis is TP2, and the ratio between both of them is ARS21/TP2.The length of the outline curve of the maximum effective half diameterposition of the image-side surface of the second lens element is denotedas ARS22, and the ratio between ARS22 and TP2 is ARS22/TP2. The ratiorelations between the lengths of the outline curve of the maximumeffective half diameter position of any surface of the other lenselements and the thicknesses of the lens elements to which the surfacesbelong on the optical axis (TP) are denoted in the similar way.

The length of outline curve of half of an entrance pupil diameter of anysurface of a single lens element especially affects the functions of thesurface aberration correction and the optical path difference in eachshared view field. The longer outline curve may lead to a betterfunction of aberration correction, but the difficulty of the productionmay become inevitable. Hence, the length of outline curve of half of anentrance pupil diameter of any surface of a single lens element has tobe controlled, and especially, the ratio relationship between the lengthof outline curve of half of an entrance pupil diameter of any surface ofa single lens element and the thickness on the optical axis has to becontrolled. For example, the length of outline curve of the half of theentrance pupil diameter of the object-side surface of the first lenselement is denoted as ARE11, and the thickness of the first lens elementon the optical axis is TP1, and the ratio thereof is ARE11/TP1. Thelength of outline curve of the half of the entrance pupil diameter ofthe image-side surface of the first lens element is denoted as ARE12,and the thickness of the first lens element on the optical axis is TP1,and the ratio thereof is ARE12/TP1. The length of outline curve of thehalf of the entrance pupil diameter of the object-side surface of thefirst lens element is denoted as ARE21, and the thickness of the secondlens element on the optical axis is TP2, and the ratio thereof isARE21/TP2. The length of outline curve of the half of the entrance pupildiameter of the image-side surface of the second lens element is denotedas ARE22, and the thickness of the second lens element on the opticalaxis is TP2, and the ratio thereof is ARE22/TP2. The ratio relationshipof the remaining lens elements of the optical image capturing system canbe referred as mentioned above.

The height of optical system (HOS) may be reduced to achieve theminimization of the optical image capturing system when the absolutevalue of f1 is larger than f6 (|f1|>f6).

When |f2|+|f3|+|f4|+|f5| and |f1|+|f6| are satisfied with aboverelations, at least one of the second through fifth lens elements mayhave weak positive refractive power or weak negative refractive power.The weak refractive power indicates that an absolute value of the focallength of a specific lens element is greater than 10. When at least oneof the second through fifth lens elements has the weak positiverefractive power, the positive refractive power of the first lenselement can be shared, such that the unnecessary aberration will notappear too early. On the contrary, when at least one of the secondthrough fifth lens elements has the weak negative refractive power, theaberration of the optical image capturing system can be corrected andfine tuned.

The sixth lens element may have negative refractive power and a concaveimage-side surface. Hereby, the back focal length is reduced for keepingthe miniaturization, to miniaturize the lens element effectively. Inaddition, at least one of the object-side surface and the image-sidesurface of the sixth lens element may have at least one inflectionpoint, such that the angle of incident with incoming light from anoff-axis view field can be suppressed effectively and the aberration inthe off-axis view field can be corrected further.

BRIEF DESCRIPTION OF THE DRAWINGS

The detailed structure, operating principle and effects of the presentdisclosure will now be described in more details hereinafter withreference to the accompanying drawings that show various embodiments ofthe present disclosure as follows.

FIG. 1A is a schematic view of the optical image capturing systemaccording to the first embodiment of the present application.

FIG. 1B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the first embodimentof the present application.

FIG. 1C is a lateral aberration diagram of tangential fan, sagittal fan,the longest operation wavelength and the shortest operation wavelengthpassing through an edge of the entrance pupil and incident on the imageplane by 0.7 HOI according to the first embodiment of the presentapplication.

FIG. 2A is a schematic view of the optical image capturing systemaccording to the second embodiment of the present application.

FIG. 2B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the secondembodiment of the present application.

FIG. 2C is a lateral aberration diagram of tangential fan, sagittal fan,the longest operation wavelength and the shortest operation wavelengthpassing through an edge of the entrance pupil and incident on the imageplane by 0.7 HOI according to the second embodiment of the presentapplication.

FIG. 3A is a schematic view of the optical image capturing systemaccording to the third embodiment of the present application.

FIG. 3B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the third embodimentof the present application.

FIG. 3C is a lateral aberration diagram of tangential fan, sagittal fan,the longest operation wavelength and the shortest operation wavelengthpassing through an edge of the entrance pupil and incident on the imageplane by 0.7 HOI according to the third embodiment of the presentapplication.

FIG. 4A is a schematic view of the optical image capturing systemaccording to the fourth embodiment of the present application.

FIG. 4B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the fourthembodiment of the present application.

FIG. 4C is a lateral aberration diagram of tangential fan, sagittal fan,the longest operation wavelength and the shortest operation wavelengthpassing through an edge of the entrance pupil and incident on the imageplane by 0.7 HOI according to the fourth embodiment of the presentapplication.

FIG. 5A is a schematic view of the optical image capturing systemaccording to the fifth embodiment of the present application.

FIG. 5B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the fifth embodimentof the present application.

FIG. 5C is a lateral aberration diagram of tangential fan, sagittal fan,the longest operation wavelength and the shortest operation wavelengthpassing through an edge of the entrance pupil and incident on the imageplane by 0.7 HOI according to the fifth embodiment of the presentapplication.

FIG. 6A is a schematic view of the optical image capturing systemaccording to the sixth embodiment of the present application.

FIG. 6B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the sixth embodimentof the present application.

FIG. 6C is a lateral aberration diagram of tangential fan, sagittal fan,the longest operation wavelength and the shortest operation wavelengthpassing through an edge of the entrance pupil and incident on the imageplane by 0.7 HOI according to the sixth embodiment of the presentapplication.

FIG. 7A is a schematic view of the optical image capturing systemaccording to the seventh embodiment of the present application.

FIG. 7B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the seventhembodiment of the present application.

FIG. 7C is a lateral aberration diagram of tangential fan, sagittal fan,the longest operation wavelength and the shortest operation wavelengthpassing through an edge of the entrance pupil and incident on the imageplane by 0.7 HOI according to the seventh embodiment of the presentapplication.

FIG. 8A is a schematic view of the optical image capturing systemaccording to the eighth embodiment of the present application.

FIG. 8B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the eighthembodiment of the present application.

FIG. 8C is a lateral aberration diagram of tangential fan, sagittal fan,the longest operation wavelength and the shortest operation wavelengthpassing through an edge of the entrance pupil and incident on the imageplane by 0.7 HOI according to the eighth embodiment of the presentapplication.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

Reference will now be made in detail to the exemplary embodiments of thepresent disclosure, examples of which are illustrated in theaccompanying drawings. Therefore, it is to be understood that theforegoing is illustrative of exemplary embodiments and is not to beconstrued as limited to the specific embodiments disclosed, and thatmodifications to the disclosed exemplary embodiments, as well as otherexemplary embodiments, are intended to be included within the scope ofthe appended claims. These embodiments are provided so that thisdisclosure will be thorough and complete, and will fully convey theinventive concept to those skilled in the art. The relative proportionsand ratios of elements in the drawings may be exaggerated or diminishedin size for the sake of clarity and convenience in the drawings, andsuch arbitrary proportions are only illustrative and not limiting in anyway. The same reference numbers are used in the drawings and thedescription to refer to the same or like parts.

It will be understood that, although the terms ‘first’, ‘second’,‘third’, etc., may be used herein to describe various elements, theseelements should not be limited by these terms. The terms are used onlyfor the purpose of distinguishing one component from another component.Thus, a first element discussed below could be termed a second elementwithout departing from the teachings of embodiments. As used herein, theterm “or” includes any and all combinations of one or more of theassociated listed items.

An optical image capturing system, in order from an object side to animage side, includes a first, second, third, fourth, fifth and sixthlens elements with refractive power and an image plane. The opticalimage capturing system may further include an image sensing device whichis disposed on an image plane.

The optical image capturing system may use three sets of wavelengthswhich are 486.1 nm, 587.5 nm and 656.2 nm, respectively, wherein 587.5nm is served as the primary reference wavelength and a referencewavelength for retrieving technical features. The optical imagecapturing system may also use five sets of wavelengths which are 470 nm,510 nm, 555 nm, 610 nm and 650 nm, respectively, wherein 555 nm isserved as the primary reference wavelength and a reference wavelengthfor retrieving technical features.

A ratio of the focal length f of the optical image capturing system to afocal length fp of each of lens elements with positive refractive poweris PPR. A ratio of the focal length f of the optical image capturingsystem to a focal length fn of each of lens elements with negativerefractive power is NPR. A sum of the PPR of all lens elements withpositive refractive power is ΣPPR. A sum of the NPR of all lens elementswith negative refractive powers is ΣNPR. It is beneficial to control thetotal refractive power and the total length of the optical imagecapturing system when following conditions are satisfied:0.5≦ΣPPR/|ΣNPR|≦15. Preferably, the following relation may be satisfied:1≦ΣPPR/|ΣNPR|≦3.0.

The optical image capturing system may further include an image sensingdevice which is disposed on an image plane. Half of a diagonal of aneffective detection field of the image sensing device (imaging height orthe maximum image height of the optical image capturing system) is HOI.A distance on the optical axis from the object-side surface of the firstlens element to the image plane is HOS. The following relations aresatisfied: HOS/HOI≦10 and 0.5≦HOS/f≦10. Preferably, the followingrelations may be satisfied: 1≦HOS/HOI≦5 and 1≦HOS/f≦7. Hereby, theminiaturization of the optical image capturing system can be maintainedeffectively, so as to be carried by lightweight portable electronicdevices.

In addition, in the optical image capturing system of the disclosure,according to different requirements, at least one aperture stop may bearranged for reducing stray light and improving the imaging quality.

In the optical image capturing system of the disclosure, the aperturestop may be a front or middle aperture. The front aperture is theaperture stop between a photographed object and the first lens element.The middle aperture is the aperture stop between the first lens elementand the image plane. If the aperture stop is the front aperture, alonger distance between the exit pupil and the image plane of theoptical image capturing system can be formed, such that more opticalelements can be disposed in the optical image capturing system and theefficiency of receiving images of the image sensing device can beraised. If the aperture stop is the middle aperture, the view angle ofthe optical image capturing system can be expended, such that theoptical image capturing system has the same advantage that is owned bywide angle cameras. A distance from the aperture stop to the image planeis InS. The following relation is satisfied: 0.2≦InS/HOS≦1.1. Hereby,the miniaturization of the optical image capturing system can bemaintained while the feature of the wild-angle lens element can beachieved.

In the optical image capturing system of the disclosure, a distance fromthe object-side surface of the first lens element to the image-sidesurface of the sixth lens element is InTL. A total central thickness ofall lens elements with refractive power on the optical axis is ΣTP. Thefollowing relation is satisfied: 0.1≦ΣTP/InTL≦0.9. Hereby, contrastratio for the image formation in the optical image capturing system anddefect-free rate for manufacturing the lens element can be givenconsideration simultaneously, and a proper back focal length is providedto dispose other optical components in the optical image capturingsystem.

A curvature radius of the object-side surface of the first lens elementis R1. A curvature radius of the image-side surface of the first lenselement is R2. The following relation is satisfied: 0.001≦|R1/R2|≦1 20.Hereby, the first lens element may have proper strength of the positiverefractive power, so as to avoid the longitudinal spherical aberrationto increase too fast. Preferably, the following relation may besatisfied: 0.01≦|R1/R2|<10.

A curvature radius of the object-side surface of the sixth lens elementis R11. A curvature radius of the image-side surface of the sixth lenselement is R12. The following relation is satisfied:−7<(R11−R12)/(R11+R12)<50. Hereby, the astigmatism generated by theoptical image capturing system can be corrected beneficially.

A distance between the first lens element and the second lens element onthe optical axis is IN12. The following relation is satisfied:IN12/f≦30. Hereby, the chromatic aberration of the lens elements can beimproved, such that the performance can be increased.

A distance between the fifth lens element and the sixth lens element onthe optical axis is IN56. The following relation is satisfied:IN56/f≦0.8. Hereby, the function of the lens elements can be improved.

Central thicknesses of the first lens element and the second lenselement on the optical axis are TP1 and TP2, respectively. The followingrelation is satisfied: 0.1≦(TP1+IN12)/TP2≦10. Hereby, the sensitivityproduced by the optical image capturing system can be controlled, andthe performance can be increased.

Central thicknesses of the fifth lens element and the sixth lens elementon the optical axis are TP5 and TP6, respectively, and a distancebetween the aforementioned two lens elements on the optical axis isIN56. The following relation is satisfied: 0.1≦(TP6+IN56)/TP5≦10.Hereby, the sensitivity produced by the optical image capturing systemcan be controlled and the total height of the optical image capturingsystem can be reduced.

Central thicknesses of the second lens element, the third lens elementand the fourth lens element on the optical axis are TP2, TP3 and TP4,respectively. A distance between the second and the third lens elementson the optical axis is IN23, and a distance between the fourth and thefifth lens elements on the optical axis is IN45. A distance between anobject-side surface of the first lens element and an image-side surfaceof sixth lens element is InTL. The following relation is satisfied:0.1≦TP4/(IN34+TP4+IN45)<1. Hereby, the aberration generated by theprocess of moving the incident light can be adjusted slightly layer uponlayer, and the total height of the optical image capturing system can bereduced.

In the optical image capturing system of the first embodiment, adistance perpendicular to the optical axis between a critical point C61on an object-side surface of the sixth lens element and the optical axisis HVT61. A distance perpendicular to the optical axis between acritical point C62 on an image-side surface of the sixth lens elementand the optical axis is HVT62. A distance in parallel with the opticalaxis from an axial point on the object-side surface of the sixth lenselement to the critical point C61 is SGC61. A distance in parallel withthe optical axis from an axial point on the image-side surface of thesixth lens element to the critical point C62 is SGC62. The followingrelations may be satisfied: 0 mm≦HVT61≦3 mm, 0 mm<HVT62≦6 mm,0≦HVT61/HVT62, 0 mm≦|SGC61≦0.5 mm; 0 mm<|SGC62|≦2 mm, and0<|SGC62/(|SGC62|+TP6)≦0.9. Hereby, the aberration of the off-axis viewfield can be corrected effectively.

The following relation is satisfied for the optical image capturingsystem of the disclosure: 0.2≦HVT62/HOI≦0.9. Preferably, the followingrelation may be satisfied: 0.3≦HVT62/HOI≦0.8. Hereby, the aberration ofsurrounding view field for the optical image capturing system can becorrected beneficially.

The following relation is satisfied for the optical image capturingsystem of the disclosure: 0≦HVT62/HOS≦0.5. Preferably, the followingrelation may be satisfied: 0.2≦HVT62/HOS≦0.45. Hereby, the aberration ofsurrounding view field for the optical image capturing system can becorrected beneficially.

In the optical image capturing system of the disclosure, a distance inparallel with an optical axis from an inflection point on theobject-side surface of the sixth lens element which is nearest to theoptical axis to an axial point on the object-side surface of the sixthlens element is denoted by SGI611. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thesixth lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the sixth lens element is denoted bySGI621. The following relations are satisfied: 0<SGI611/(SGI611+TP6)≦0.9and 0<SGI621/(SGI621+TP6)≦0.9. Preferably, the following relations maybe satisfied: 0.1≦SGI611/(SGI611+TP6)≦0.6 and0.1≦SGI621/(SGI621+TP6)≦0.6.

A distance in parallel with the optical axis from the inflection pointon the object-side surface of the sixth lens element which is the secondnearest to the optical axis to an axial point on the object-side surfaceof the sixth lens element is denoted by SGI612. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the sixth lens element which is the second nearest to the opticalaxis to an axial point on the image-side surface of the sixth lenselement is denoted by SGI622. The following relations are satisfied:0<SGI612/(SGI612+TP6)≦0.9 and 0<SGI622/(SGI622+TP6)≦0.9. Preferably, thefollowing relations may be satisfied: 0.1≦SGI612/(SGI612+TP6)≦0.6 and0.1≦SGI622/(SGI622+TP6)≦0.6.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which is thenearest to the optical axis and the optical axis is denoted by HIF611. Adistance perpendicular to the optical axis between an axial point on theimage-side surface of the sixth lens element and an inflection point onthe image-side surface of the sixth lens element which is the nearest tothe optical axis is denoted by HIF621. The following relations aresatisfied: 0.001 mm≦|HIF611|≦5 mm and 0.001 mm≦|HIF621|≦5 mm.Preferably, the following relations may be satisfied: 0.1mm≦|HIF611|≦3.5 mm and 1.5≦|HIF621|≦3.5 mm.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which is thesecond nearest to the optical axis and the optical axis is denoted byHIF612. A distance perpendicular to the optical axis between an axialpoint on the image-side surface of the sixth lens element and aninflection point on the image-side surface of the sixth lens elementwhich is the second nearest to the optical axis is denoted by HIF622.The following relations are satisfied: 0.001 mm≦|HIF612|≦5 mm and 0.001mm≦|HIF622|≦5 mm. Preferably, the following relations may be satisfied:0.1 mm≦|HIF622|≦3.5 mm and 0.1 mm≦|HIF612|≦3.5 mm.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which is thethird nearest to the optical axis and the optical axis is denoted byHIF613. A distance perpendicular to the optical axis between an axialpoint on the image-side surface of the sixth lens element and aninflection point on the image-side surface of the sixth lens elementwhich is the third nearest to the optical axis is denoted by HIF623. Thefollowing relations are satisfied: 0.001 mm≦|HIF613 5 mm and 0.001mm≦|HIF623|≦5 mm. Preferably, the following relations may be satisfied:0.1 mm≦|HIF623|≦3.5 mm and 0.1 mm≦|HIF613|≦3.5 mm.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which is thefourth nearest to the optical axis and the optical axis is denoted byHIF614. A distance perpendicular to the optical axis between an axialpoint on the image-side surface of the sixth lens element and aninflection point on the image-side surface of the sixth lens elementwhich is the fourth nearest to the optical axis is denoted by HIF624.The following relations are satisfied: 0.001 mm≦|HIF614|≦5 mm and 0.001mm≦|HIF624|≦5 mm. Preferably, the following relations may be satisfied:0.1 mm≦|HIF624|≦3.5 mm and 0.1 mm≦|HIF614|≦3.5 mm.

In one embodiment of the optical image capturing system of the presentdisclosure, the chromatic aberration of the optical image capturingsystem can be corrected by alternatively arranging the lens elementswith large Abbe number and small Abbe number.

The above Aspheric formula is:

z=ch ²/[1+[1−(k+1)c ² h ²]^(0.5) ]+A4h ⁴ +A6h ⁶ +A8h ⁸ +A10h ¹⁰ +A12h ¹²+A14h ¹⁴ +A16h ¹⁶ +A18h ¹⁸ +A20h ²⁰+ . . .   (1),

where z is a position value of the position along the optical axis andat the height h which reference to the surface apex; k is the coniccoefficient, c is the reciprocal of curvature radius, and A4, A6, A8,A10, A12, A14, A16, A18, and A20 are high order aspheric coefficients.

The optical image capturing system provided by the disclosure, the lenselements may be made of glass or plastic material. If plastic materialis adopted to produce the lens elements, the cost of manufacturing willbe lowered effectively. If lens elements are made of glass, the heateffect can be controlled and the designed space arranged for therefractive power of the optical image capturing system can be increased.Besides, the object-side surface and the image-side surface of the firstthrough sixth lens elements may be aspheric, so as to obtain morecontrol variables. Comparing with the usage of traditional lens elementmade by glass, the number of lens elements used can be reduced and theaberration can be eliminated. Thus, the total height of the opticalimage capturing system can be reduced effectively.

In addition, in the optical image capturing system provided by thedisclosure, if the lens element has a convex surface, the surface of thelens element adjacent to the optical axis is convex in principle. If thelens element has a concave surface, the surface of the lens elementadjacent to the optical axis is concave in principle.

The optical image capturing system of the disclosure can be adapted tothe optical image capturing system with automatic focus if required.With the features of a good aberration correction and a high quality ofimage formation, the optical image capturing system can be used invarious application fields.

The optical image capturing system of the disclosure can include adriving module according to the actual requirements. The driving modulemay be coupled with the lens elements to enable the lens elementsproducing displacement. The driving module may be the voice coil motor(VCM) which is applied to move the lens to focus, or may be the opticalimage stabilization (OIS) which is applied to reduce the distortionfrequency owing to the vibration of the lens while shooting.

At least one of the first, second, third, fourth, fifth and sixth lenselements of the optical image capturing system of the disclosure mayfurther be designed as a light filtration element with a wavelength ofless than 500 nm according to the actual requirement. The light filterelement may be made by coating at least one surface of the specific lenselement characterized of the filter function, and alternatively, may bemade by the lens element per se made of the material which is capable offiltering short wavelength.

According to the above embodiments, the specific embodiments withfigures are presented in detail as below.

The First Embodiment (Embodiment 1)

Please refer to FIG. 1A and FIG. 1B. FIG. 1A is a schematic view of theoptical image capturing system according to the first embodiment of thepresent application, FIG. 1B is longitudinal spherical aberrationcurves, astigmatic field curves, and an optical distortion curve of theoptical image capturing system in the order from left to right accordingto the first embodiment of the present application, and FIG. 1C is alateral aberration diagram of tangential fan, sagittal fan, the longestoperation wavelength and the shortest operation wavelength passingthrough an edge of the entrance pupil and incident on the image plane by0.7 HOI according to the first embodiment of the present application. Asshown in FIG. 1A, in order from an object side to an image side, theoptical image capturing system includes a first lens element 110, anaperture stop 100, a second lens element 120, a third lens element 130,a fourth lens element 140, a fifth lens element 150, a sixth lenselement 160, an IR-bandstop filter 180, an image plane 190, and an imagesensing device 192.

The first lens element 110 has negative refractive power and it is madeof plastic material. The first lens element 110 has a concaveobject-side surface 112 and a concave image-side surface 114, both ofthe object-side surface 112 and the image-side surface 114 are aspheric,and the object-side surface 112 has two inflection points. The length ofoutline curve of the maximum effective half diameter position of theobject-side surface of the first lens element is denoted as ARS11. Thelength of outline curve of the maximum effective half diameter positionof the image-side surface of the first lens element is denoted as ARS12.The length of outline curve of a half of an entrance pupil diameter(HEP) of the object-side surface of the first lens element is denoted asARE11, and the length of outline curve of the half of the entrance pupildiameter (HEP) of the image-side surface of the first lens element isdenoted as ARE12. The thickness of the first lens element on the opticalaxis is TP1.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the first lens element which is nearest tothe optical axis to an axial point on the object-side surface of thefirst lens element is denoted by SGI111. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thefirst lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the first lens element is denoted bySGI121. The following relations are satisfied: SGI111=−0.0031 mm andSGI111|/(|SGI111|+TP1)=0.0016.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the first lens element which is the secondnearest to the optical axis to an axial point on the object-side surfaceof the first lens element is denoted by SGI112. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the first lens element which is the second nearest to the opticalaxis to an axial point on the image-side surface of the first lenselement is denoted by SGI122. The following relations are satisfied:SGI112=1.3178 mm and |SGI112|/(|SGI112+TP1)=0.4052.

A distance perpendicular to the optical axis from the inflection pointon the object-side surface of the first lens element which is nearest tothe optical axis to an axial point on the object-side surface of thefirst lens element is denoted by HIF 111. A distance perpendicular tothe optical axis from the inflection point on the image-side surface ofthe first lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the first lens element is denoted byHIF121. The following relations are satisfied: HIF111=0.5557 mm andHIF111/HOI=0.1111.

A distance perpendicular to the optical axis from the inflection pointon the object-side surface of the first lens element which is the secondnearest to the optical axis to an axial point on the object-side surfaceof the first lens element is denoted by HIF112. A distance perpendicularto the optical axis from the inflection point on the image-side surfaceof the first lens element which is the second nearest to the opticalaxis to an axial point on the image-side surface of the first lenselement is denoted by HIF121. The following relations are satisfied:HIF112=5.3732 mm and HIF112/HOI=1.0746.

The second lens element 120 has positive refractive power and it is madeof plastic material. The second lens element 120 has a convexobject-side surface 122 and a convex image-side surface 124, and both ofthe object-side surface 122 and the image-side surface 124 are aspheric.The object-side surface 122 has an inflection point. The length ofoutline curve of the maximum effective half diameter position of theobject-side surface of the second lens element is denoted as ARS21, andthe length of outline curve of the maximum effective half diameterposition of the image-side surface of the second lens element is denotedas ARS22. The length of outline curve of a half of an entrance pupildiameter (HEP) of the object-side surface of the second lens element isdenoted as ARE21, and the length of outline curve of the half of theentrance pupil diameter (HEP) of the image-side surface of the secondlens element is denoted as ARS22. The thickness of the second lenselement on the optical axis is TP2.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the second lens element which is nearest tothe optical axis to an axial point on the object-side surface of thesecond lens element is denoted by SGI211. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thesecond lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the second lens element is denoted bySGI221. The following relations are satisfied: SGI211=0.1069 mm,|SGI211|/(|SGI211+TP2)=0.0412, SGI221=0 mm and|SGI221|/(|SGI221|+TP2)=0.

A distance perpendicular to the optical axis from the inflection pointon the object-side surface of the second lens element which is nearestto the optical axis to an axial point on the object-side surface of thesecond lens element is denoted by HIF211. A distance perpendicular tothe optical axis from the inflection point on the image-side surface ofthe second lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the second lens element is denoted byHIF221. The following relations are satisfied: HIF211=1.1264 mm,HIF211/HOI=0.2253, HIF221=0 mm and HIF221/HOI=0.

The third lens element 130 has negative refractive power and it is madeof plastic material. The third lens element 130 has a concaveobject-side surface 132 and a convex image-side surface 134, and both ofthe object-side surface 132 and the image-side surface 134 are aspheric.The object-side surface 132 and the image-side surface 134 both have aninflection point. The length of outline curve of the maximum effectivehalf diameter position of the object-side surface of the third lenselement is denoted as ARS31, and the length of outline curve of themaximum effective half diameter position of the image-side surface ofthe third lens element is denoted as ARS32. The length of outline curveof a half of an entrance pupil diameter (HEP) of the object-side surfaceof the third lens element is denoted as ARE31, and the length of outlinecurve of the half of the entrance pupil diameter (HEP) of the image-sidesurface of the third lens element is denoted as ARS32. The thickness ofthe third lens element on the optical axis is TP3.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the third lens element which is nearest tothe optical axis to an axial point on the object-side surface of thethird lens element is denoted by SGI311. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thethird lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the third lens element is denoted bySGI321. The following relations are satisfied: SGI311=−0.3041 mm,|SGI311|/(|SGI311|+TP3)=0.4445, SGI321=−0.1172 mm and|SGI321|/(|SGI321|+TP3)=0.2357.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the third lens element which isnearest to the optical axis and the optical axis is denoted by HIF311. Adistance perpendicular to the optical axis from the inflection point onthe image-side surface of the third lens element which is nearest to theoptical axis to an axial point on the image-side surface of the thirdlens element is denoted by HIF321. The following relations aresatisfied: HIF311=1.5907 mm, HIF311/HOI=0.3181, HIF321=1.3380 mm andHIF321/HOI=0.2676.

The fourth lens element 140 has positive refractive power and it is madeof plastic material. The fourth lens element 140 has a convexobject-side surface 142 and a concave image-side surface 144, both ofthe object-side surface 142 and the image-side surface 144 are aspheric,the object-side surface 142 has two inflection points, and theimage-side surface 144 has an inflection point. The length of outlinecurve of the maximum effective half diameter position of the object-sidesurface of the fourth lens element is denoted as ARS41, and the lengthof outline curve of the maximum effective half diameter position of theimage-side surface of the fourth lens element is denoted as ARS42. Thelength of outline curve of a half of an entrance pupil diameter (HEP) ofthe object-side surface of the fourth lens element is denoted as ARE41,and the length of outline curve of the half of the entrance pupildiameter (HEP) of the image-side surface of the fourth lens element isdenoted as ARS42. The thickness of the fourth lens element on theoptical axis is TP4.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the fourth lens element which is nearest tothe optical axis to an axial point on the object-side surface of thefourth lens element is denoted by SGI411. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thefourth lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the fourth lens element is denoted bySGI421. The following relations are satisfied: SGI411=0.0070 mm,|SGI411|/(|SGI411|+TP4)=0.0056, SGI421=0.0006 mm and|SGI421|/(|SGI421|+TP4)=0.0005.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the fourth lens element which is the secondnearest to the optical axis to an axial point on the object-side surfaceof the fourth lens element is denoted by SGI412. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the fourth lens element which is the second nearest to the opticalaxis to an axial point on the image-side surface of the fourth lenselement is denoted by SGI422. The following relations are satisfied:SGI412=−0.2078 mm and |SGI412|/(|SGI412|+TP4)=0.1439.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fourth lens element which isnearest to the optical axis and the optical axis is denoted by HIF411. Adistance perpendicular to the optical axis between the inflection pointon the image-side surface of the fourth lens element which is nearest tothe optical axis and the optical axis is denoted by HIF421. Thefollowing relations are satisfied: HIF411=0.4706 mm, HIF411/HOI=0.0941,HIF421=0.1721 mm and HIF421/HOI=0.0344.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fourth lens element which is thesecond nearest to the optical axis and the optical axis is denoted byHIF412. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the fourth lens elementwhich is the second nearest to the optical axis and the optical axis isdenoted by HIF422. The following relations are satisfied: HIF412=2.0421mm and HIF412/HOI=0.4084.

The fifth lens element 150 has positive refractive power and it is madeof plastic material. The fifth lens element 150 has a convex object-sidesurface 152 and a convex image-side surface 154, and both of theobject-side surface 152 and the image-side surface 154 are aspheric. Theobject-side surface 152 has two inflection points and the image-sidesurface 154 has an inflection point. The length of outline curve of themaximum effective half diameter position of the object-side surface ofthe fifth lens element is denoted as ARS51, and the length of outlinecurve of the maximum effective half diameter position of the image-sidesurface of the fifth lens element is denoted as ARS52. The length ofoutline curve of a half of an entrance pupil diameter (HEP) of theobject-side surface of the fifth lens element is denoted as ARE51, andthe length of outline curve of the half of the entrance pupil diameter(HEP) of the image-side surface of the fifth lens element is denoted asARE52. The thickness of the fifth lens element on the optical axis isTP5.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the fifth lens element which is nearest tothe optical axis to an axial point on the object-side surface of thefifth lens element is denoted by SGI511. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thefifth lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the fifth lens element is denoted bySGI521. The following relations are satisfied: SGI511=0.00364 mm,|SGI511|/(|SGI511|+TP5)=0.00338, SGI521=−0.63365 mm and|SGI521|/(|SGI521|+TP5)=0.37154.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the fifth lens element which is the secondnearest to the optical axis to an axial point on the object-side surfaceof the fifth lens element is denoted by SGI512. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the fifth lens element which is the second nearest to the opticalaxis to an axial point on the image-side surface of the fifth lenselement is denoted by SGI522. The following relations are satisfied:SGI512=−0.32032 mm and |SGI512|/(|SGI512|+TP5)=0.23009.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the fifth lens element which is the thirdnearest to the optical axis to an axial point on the object-side surfaceof the fifth lens element is denoted by SGI513. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the fifth lens element which is the third nearest to the optical axisto an axial point on the image-side surface of the fifth lens element isdenoted by SGI523. The following relations are satisfied: SGI513=0 mm,|SGI513|/(|SGI513|+TP5)=0, SGI523=0 mm and |SGI523|/(|SGI523|+TP5)=0.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the fifth lens element which is the fourthnearest to the optical axis to an axial point on the object-side surfaceof the fifth lens element is denoted by SGI514. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the fifth lens element which is the fourth nearest to the opticalaxis to an axial point on the image-side surface of the fifth lenselement is denoted by SGI524. The following relations are satisfied:SGI514=0 mm, |SGI514|/(|SGI514|+TP5)=0, SGI524=0 mm and|SGI524|/(|SGI524|+TP5)=0.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fifth lens element which isnearest to the optical axis and the optical axis is denoted by HIF511. Adistance perpendicular to the optical axis between the inflection pointon the image-side surface of the fifth lens element which is nearest tothe optical axis and the optical axis is denoted by HIF521. Thefollowing relations are satisfied: HIF511=0.28212 mm,HIF511/HOI=0.05642, HIF521=2.13850 mm and HIF521/HOI=0.42770.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fifth lens element which is thesecond nearest to the optical axis and the optical axis is denoted byHIF512. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the fifth lens elementwhich is the second nearest to the optical axis and the optical axis isdenoted by HIF522. The following relations are satisfied: HIF512=2.51384mm and HIF512/HOI=0.50277.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fifth lens element which is thethird nearest to the optical axis and the optical axis is denoted byHIF513. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the fifth lens elementwhich is the third nearest to the optical axis and the optical axis isdenoted by HIF523. The following relations are satisfied: HIF513=0 mm,HIF513/HOI=0, HIF523=0 mm and HIF523/HOI=0.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fifth lens element which is thefourth nearest to the optical axis and the optical axis is denoted byHIF514. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the fifth lens elementwhich is the fourth nearest to the optical axis and the optical axis isdenoted by HIF524. The following relations are satisfied: HIF514=0 mm,HIF514/HOI=0, HIF524=0 mm and HIF524/HOI=0.

The sixth lens element 160 has negative refractive power and it is madeof plastic material. The sixth lens element 160 has a concaveobject-side surface 162 and a concave image-side surface 164, and theobject-side surface 162 has two inflection points and the image-sidesurface 164 has an inflection point. Hereby, the angle of incident ofeach view field on the sixth lens element can be effectively adjustedand the spherical aberration can thus be improved. The length of outlinecurve of the maximum effective half diameter position of the object-sidesurface of the sixth lens element is denoted as ARS61, and the length ofoutline curve of the maximum effective half diameter position of theimage-side surface of the sixth lens element is denoted as ARS62. Thelength of outline curve of a half of an entrance pupil diameter (HEP) ofthe object-side surface of the sixth lens element is denoted as ARE61,and the length of outline curve of the half of the entrance pupildiameter (HEP) of the image-side surface of the sixth lens element isdenoted as ARE62. The thickness of the sixth lens element on the opticalaxis is TP6.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the sixth lens element which is nearest tothe optical axis to an axial point on the object-side surface of thesixth lens element is denoted by SGI611. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thesixth lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the sixth lens element is denoted bySGI621. The following relations are satisfied: SGI611=−0.38558 mm,|SGI611|/(|SGI611|+TP6)=0.27212, SGI621=0.12386 mm and|SGI621|/(|SGI621|+TP6)=0.10722.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the sixth lens element which is the secondnearest to the optical axis to an axial point on the object-side surfaceof the sixth lens element is denoted by SGI612. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the sixth lens element which is the second nearest to the opticalaxis to an axial point on the image-side surface of the sixth lenselement is denoted by SGI622. The following relations are satisfied:SGI612=−0.47400 mm, |SGI612|/(|SGI612|+TP6)=0.31488, SGI622=0 mm and|SGI622|/(|SGI622|+TP6)=0.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which isnearest to the optical axis and the optical axis is denoted by HIF611. Adistance perpendicular to the optical axis between the inflection pointon the image-side surface of the sixth lens element which is nearest tothe optical axis and the optical axis is denoted by HIF621. Thefollowing relations are satisfied: HIF611=2.24283 mm,HIF611/HOI=0.44857, HIF621=1.07376 mm and HIF621/HOI=0.21475.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which is thesecond nearest to the optical axis and the optical axis is denoted byHIF612. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the sixth lens elementwhich is the second nearest to the optical axis and the optical axis isdenoted by HIF622. The following relations are satisfied: HIF612=2.48895mm and HIF612/HOI=0.49779.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which is thethird nearest to the optical axis and the optical axis is denoted byHIF613. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the sixth lens elementwhich is the third nearest to the optical axis and the optical axis isdenoted by HIF623. The following relations are satisfied: HIF613=0 mm,HIF613/HOI=0, HIF623=0 mm and HIF623/HOI=0.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which is thefourth nearest to the optical axis and the optical axis is denoted byHIF614. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the sixth lens elementwhich is the fourth nearest to the optical axis and the optical axis isdenoted by HIF624. The following relations are satisfied: HIF614=0 mm,HIF614/HOI=0, HIF624=0 mm and HIF624/HOI=0.

The IR-bandstop filter 180 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 160 and the image plane 190.

In the optical image capturing system of the first embodiment, a focallength of the optical image capturing system is f, an entrance pupildiameter of the optical image capturing system is HEP, and half of amaximum view angle of the optical image capturing system is HAF. Thedetailed parameters are shown as below: f=4.075 mm, f/HEP=1.4,HAF=50.001° and tan(HAF)=1.1918.

In the optical image capturing system of the first embodiment, a focallength of the first lens element 110 is f1 and a focal length of thesixth lens element 160 is f6. The following relations are satisfied:f1=−7.828 mm, |f/f1|=0.52060, f6=−4.886 and |f1|>|f6|.

In the optical image capturing system of the first embodiment, focallengths of the second lens element 120 to the fifth lens element 150 aref2, f3, f4 and f5, respectively. The following relations are satisfied:|f2|+|f3|+|f4|+|f5|=95.50815 mm, |f1|+|f6|=12.71352 mm and|f2|+|f3|+|f4|+|f5|>|f1|+|f6|.

A ratio of the focal length f of the optical image capturing system to afocal length fp of each of lens elements with positive refractive poweris PPR. A ratio of the focal length f of the optical image capturingsystem to a focal length fn of each of lens elements with negativerefractive power is NPR. In the optical image capturing system of thefirst embodiment, a sum of the PPR of all lens elements with positiverefractive power is ΣPPR=f/f1+f/f3+f/f5=1.63290. A sum of the NPR of alllens elements with negative refractive powers isΣNPR=f/f1|+|f/f3|+|f/f6=1.51305, ΣPPR/|ΣNPR|=1.07921. The followingrelations are also satisfied: f/f2|=0.69101, |f/f3|=0.15834,|f/f4|=0.06883, |f/f5=0.87305 and |f/f6|=0.83412.

In the optical image capturing system of the first embodiment, adistance from the object-side surface 112 of the first lens element tothe image-side surface 164 of the sixth lens element is InTL. A distancefrom the object-side surface 112 of the first lens element to the imageplane 190 is HOS. A distance from an aperture 100 to an image plane 190is InS. Half of a diagonal length of an effective detection field of theimage sensing device 192 is HOI. A distance from the image-side surface164 of the sixth lens element to the image plane 190 is BFL. Thefollowing relations are satisfied: InTL+BFL=HOS, HOS=19.54120 mm,HOI=5.0 mm, HOS/HOI=3.90824, HOS/f=4.7952, InS=11.685 mm andInS/HOS=0.59794.

In the optical image capturing system of the first embodiment, a totalcentral thickness of all lens elements with refractive power on theoptical axis is ΣTP. The following relations are satisfied: ΣTP=8.13899mm and ΣTP/InTL=0.52477. Hereby, contrast ratio for the image formationin the optical image capturing system and defect-free rate formanufacturing the lens element can be given considerationsimultaneously, and a proper back focal length is provided to disposeother optical components in the optical image capturing system.

In the optical image capturing system of the first embodiment, acurvature radius of the object-side surface 112 of the first lenselement is R1. A curvature radius of the image-side surface 114 of thefirst lens element is R2. The following relation is satisfied:|R1/R2|=8.99987. Hereby, the first lens element may have proper strengthof the positive refractive power, so as to avoid the longitudinalspherical aberration to increase too fast.

In the optical image capturing system of the first embodiment, acurvature radius of the object-side surface 162 of the sixth lenselement is R11. A curvature radius of the image-side surface 164 of thesixth lens element is R12. The following relation is satisfied:(R11−R12)/(R11+R12)=1.27780. Hereby, the astigmatism generated by theoptical image capturing system can be corrected beneficially.

In the optical image capturing system of the first embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relations are satisfied: ΣPP=f2+f4+f5=69.770 mm andf5/(f2+f4+f5)=0.067. Hereby, it is favorable for allocating the positiverefractive power of the first lens element 110 to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the first embodiment, a sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relations are satisfied: ΣNP=f1+f3+f6=−38.451 mm andf6/(f1+f3+f6)=0.127. Hereby, it is favorable for allocating the negativerefractive power of the sixth lens element 160 to other negative lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the first embodiment, adistance between the first lens element 110 and the second lens element120 on the optical axis is IN12. The following relations are satisfied:IN12=6.418 mm and IN12/f=1.57491. Hereby, the chromatic aberration ofthe lens elements can be improved, such that the performance can beincreased.

In the optical image capturing system of the first embodiment, adistance between the fifth lens element 150 and the sixth lens element160 on the optical axis is IN56. The following relations are satisfied:IN56=0.025 mm and IN56/f=0.00613. Hereby, the chromatic aberration ofthe lens elements can be improved, such that the performance can beincreased.

In the optical image capturing system of the first embodiment, centralthicknesses of the first lens element 110 and the second lens element120 on the optical axis are TP1 and TP2, respectively. The followingrelations are satisfied: TP1=1.934 mm, TP2=2.486 mm and(TP1+IN12)/TP2=3.36005. Hereby, the sensitivity produced by the opticalimage capturing system can be controlled, and the performance can beincreased.

In the optical image capturing system of the first embodiment, centralthicknesses of the fifth lens element 150 and the sixth lens element 160on the optical axis are TP5 and TP6, respectively, and a distancebetween the aforementioned two lens elements on the optical axis isIN56. The following relations are satisfied: TP5=1.072 mm, TP6=1.031 mmand (TP6+IN56)/TP5=0.98555. Hereby, the sensitivity produced by theoptical image capturing system can be controlled and the total height ofthe optical image capturing system can be reduced.

In the optical image capturing system of the first embodiment, adistance between the third lens element 130 and the fourth lens element140 on the optical axis is IN34. A distance between the fourth lenselement 140 and the fifth lens element 150 on the optical axis is IN45.The following relations are satisfied: IN34=0.401 mm, IN45=0.025 mm andTP4/(IN34+TP4+IN45)=0.74376. Hereby, the aberration generated by theprocess of moving the incident light can be adjusted slightly layer uponlayer, and the total height of the optical image capturing system can bereduced.

In the optical image capturing system of the first embodiment, adistance in parallel with an optical axis from a maximum effective halfdiameter position to an axial point on the object-side surface 152 ofthe fifth lens element is InRS51. A distance in parallel with an opticalaxis from a maximum effective half diameter position to an axial pointon the image-side surface 154 of the fifth lens element is InRS52. Acentral thickness of the fifth lens element 150 is TP5. The followingrelations are satisfied: InRS51=−0.34789 mm, InRS52=−0.88185 mm,|InRS51□/TP5=0.32458 and |InRS52□/TP5=0.82276. Hereby, it is favorablefor manufacturing and forming the lens element and for maintaining theminimization for the optical image capturing system.

In the optical image capturing system of the first embodiment, adistance perpendicular to the optical axis between a critical point C51on the object-side surface 152 of the fifth lens element and the opticalaxis is HVT51. A distance perpendicular to the optical axis between acritical point C52 on the image-side surface 154 of the fifth lenselement and the optical axis is HVT52. The following relations aresatisfied: HVT51=0.515349 mm and HVT52=0 mm.

In the optical image capturing system of the first embodiment, adistance in parallel with an optical axis from a maximum effective halfdiameter position to an axial point on the object-side surface 162 ofthe sixth lens element is InRS61. A distance in parallel with an opticalaxis from a maximum effective half diameter position to an axial pointon the image-side surface 164 of the sixth lens element is InRS62. Acentral thickness of the sixth lens element 160 is TP6. The followingrelations are satisfied: InRS61=−0.58390 mm, InRS62=0.41976 mm,InRS61□/TP6=0.56616 and |InRS62□/TP6=0.40700. Hereby, it is favorablefor manufacturing and forming the lens element and for maintaining theminimization for the optical image capturing system.

In the optical image capturing system of the first embodiment, adistance perpendicular to the optical axis between a critical point C61on the object-side surface 162 of the sixth lens element and the opticalaxis is HVT61. A distance perpendicular to the optical axis between acritical point C62 on the image-side surface 164 of the sixth lenselement and the optical axis is HVT62. The following relations aresatisfied: HVT61=0 mm and HVT62=0 mm.

In the optical image capturing system of the first embodiment, thefollowing relation is satisfied: HVT51/HOI=0.1031. Hereby, theaberration of surrounding view field can be corrected.

In the optical image capturing system of the first embodiment, thefollowing relation is satisfied: HVT51/HOS=0.02634. Hereby, theaberration of surrounding view field can be corrected.

In the optical image capturing system of the first embodiment, thesecond lens element 120, the third lens element 130 and the sixth lenselement 160 have negative refractive power. An Abbe number of the secondlens element is NA2. An Abbe number of the third lens element is NA3. AnAbbe number of the sixth lens element is NA6. The following relation issatisfied: NA6/NA2≦1. Hereby, the chromatic aberration of the opticalimage capturing system can be corrected.

In the optical image capturing system of the first embodiment, TVdistortion and optical distortion for image formation in the opticalimage capturing system are TDT and ODT, respectively. The followingrelations are satisfied: |TDT|=2.124% and |ODT|=5.076%.

In the optical image capturing system of the first embodiment, a lateralaberration of the longest operation wavelength of a visible light of apositive direction tangential fan of the optical image capturing systempassing through an edge of the aperture and incident on the image planeby 0.7 view field is denoted as PLTA, which is 0.006 mm. A lateralaberration of the shortest operation wavelength of a visible light ofthe positive direction tangential fan of the optical image capturingsystem passing through the edge of the aperture and incident on theimage plane by 0.7 view field is denoted as PSTA, which is 0.005 mm. Alateral aberration of the longest operation wavelength of a visiblelight of a negative direction tangential fan of the optical imagecapturing system passing through the edge of the aperture and incidenton the image plane by 0.7 view field is denoted as NLTA, which is 0.004mm. A lateral aberration of the shortest operation wavelength of avisible light of a negative direction tangential fan of the opticalimage capturing system passing through the edge of the aperture andincident on the image plane by 0.7 view field is denoted as NSTA, whichis −0.007 mm. A lateral aberration of the longest operation wavelengthof a visible light of a sagittal fan of the optical image capturingsystem passing through the edge of the aperture and incident on theimage plane by 0.7 view field is denoted as SLTA, which is −0.003 mm. Alateral aberration of the shortest operation wavelength of a visiblelight of the sagittal fan of the optical image capturing system passingthrough the edge of the aperture and incident on the image plane by 0.7view field is denoted as SSTA, which is 0.008 mm.

Please refer to the following Table 1 and Table 2.

The detailed data of the optical image capturing system of the firstembodiment is as shown in Table 1.

TABLE 1 Data of the optical image capturing system f = 4.075 mm, f/HEP =1.4, HAF = 50.000 deg Focal Surface # Curvature Radius ThicknessMaterial Index Abbe # length 0 Object Plano Plano 1 Lens 1 −40.996257041.934 Plastic 1.515 56.55 −7.828 2 4.555209289 5.923 3 Ape. stop Plano0.495 4 Lens 2 5.333427366 2.486 Plastic 1.544 55.96 5.897 5−6.781659971 0.502 6 Lens 3 −5.697794287 0.380 Plastic 1.642 22.46−25.738 7 −8.883957518 0.401 8 Lens 4 13.19225664 1.236 Plastic 1.54455.96 59.205 9 21.55681832 0.025 10 Lens 5 8.987806345 1.072 Plastic1.515 56.55 4.668 11 −3.158875374 0.025 12 Lens 6 −29.46491425 1.031Plastic 1.642 22.46 −4.886 13 3.593484273 2.412 14 IR-bandstop Plano0.200 1.517 64.13 filter 15 Plano 1.420 16 Image plane Plano Referencewavelength (d-line) = 555 nm; shield position: The clear aperture of thefirst surface is 5.800 mm. The clear aperture of the third surface is1.570 mm. The clear aperture of the fifth surface is 1.950 mm.As for the parameters of the aspheric surfaces of the first embodiment,reference is made to

TABLE 2 Aspheric Coefficients Surface # 1 2 4 5 6 7 8 k 4.310876E+01−4.707622E+00 2.616025E+00 2.445397E+00 5.645686E+00 −2.117147E+01−5.287220E+00 A4 7.054243E−03 1.714312E−02 −8.377541E−03 −1.789549E−02−3.379055E−03 −1.370959E−02 −2.937377E−02 A6 −5.233264E−04 −1.502232E−04−1.838068E−03 −3.657520E−03 −1.225453E−03 6.250200E−03 2.743532E−03 A83.077890E−05 −1.359611E−04 1.233332E−03 −1.131622E−03 −5.979572E−03−5.854426E−03 −2.457574E−03 A10 −1.260650E−06 2.680747E−05 −2.390895E−031.390351E−03 4.556449E−03 4.049451E−03 1.874319E−03 A12 3.319093E−08−2.017491E−06 1.998555E−03 −4.152857E−04 −1.177175E−03 −1.314592E−03−6.013661E−04 A14 −5.051600E−10 6.604615E−08 −9.734019E−04 5.487286E−051.370522E−04 2.143097E−04 8.792480E−05 A16 3.380000E−12 −1.301630E−092.478373E−04 −2.919339E−06 −5.974015E−06 −1.399894E−05 −4.770527E−06Surface # 9 10 11 12 13 k 6.200000E+01 −2.114008E+01 −7.699904E+00−6.155476E+01 −3.120467E−01 A4 −1.359965E−01 −1.263831E−01 −1.927804E−02−2.492467E−02 −3.521844E−02 A6 6.628518E−02 6.965399E−02 2.478376E−03−1.835360E−03 5.629654E−03 A8 −2.129167E−02 −2.116027E−02 1.438785E−033.201343E−03 −5.466925E−04 A10 4.396344E−03 3.819371E−03 −7.013749E−04−8.990757E−04 2.231154E−05 A12 −5.542899E−04 −4.040283E−04 1.253214E−041.245343E−04 5.548990E−07 A14 3.768879E−05 2.280473E−05 −9.943196E−06−8.788363E−06 −9.396920E−08 A16 −1.052467E−06 −5.165452E−07 2.898397E−072.494302E−07 2.728360E−09

The numerical related to the length of outline curve is shown accordingto table 1 and table 2.

First embodiment (Reference wavelength = 555 nm) ARE 1/2(HEP) ARE valueARE − 1/2(HEP) 2(ARE/HEP) % TP ARE/TP (%) 11 1.455 1.455 −0.00033 99.98%1.934 75.23% 12 1.455 1.495 0.03957 102.72% 1.934 77.29% 21 1.455 1.4650.00940 100.65% 2.486 58.93% 22 1.455 1.495 0.03950 102.71% 2.486 60.14%31 1.455 1.486 0.03045 102.09% 0.380 391.02% 32 1.455 1.464 0.00830100.57% 0.380 385.19% 41 1.455 1.458 0.00237 100.16% 1.236 117.95% 421.455 1.484 0.02825 101.94% 1.236 120.04% 51 1.455 1.462 0.00672 100.46%1.072 136.42% 52 1.455 1.499 0.04335 102.98% 1.072 139.83% 61 1.4551.465 0.00964 100.66% 1.031 142.06% 62 1.455 1.469 0.01374 100.94% 1.031142.45% ARS EHD ARS value ARS − EHD (ARS/EHD) % TP ARS/TP (%) 11 5.8006.141 0.341 105.88% 1.934 317.51% 12 3.299 4.423 1.125 134.10% 1.934228.70% 21 1.664 1.674 0.010 100.61% 2.486 67.35% 22 1.950 2.119 0.169108.65% 2.486 85.23% 31 1.980 2.048 0.069 103.47% 0.380 539.05% 32 2.0842.101 0.017 100.83% 0.380 552.87% 41 2.247 2.287 0.040 101.80% 1.236185.05% 42 2.530 2.813 0.284 111.22% 1.236 227.63% 51 2.655 2.690 0.035101.32% 1.072 250.99% 52 2.764 2.930 0.166 106.00% 1.072 273.40% 612.816 2.905 0.089 103.16% 1.031 281.64% 62 3.363 3.391 0.029 100.86%1.031 328.83%

Table 1 is the detailed structure data to the first embodiment in FIG.1A, wherein the unit of the curvature radius, the thickness, thedistance, and the focal length is millimeters (mm). Surfaces 0-16illustrate the surfaces from the object side to the image plane in theoptical image capturing system. Table 2 is the aspheric coefficients ofthe first embodiment, wherein k is the conic coefficient in the asphericsurface formula, and A1-A20 are the first to the twentieth orderaspheric surface coefficient. Besides, the tables in the followingembodiments are referenced to the schematic view and the aberrationgraphs, respectively, and definitions of parameters in the tables areequal to those in the Table 1 and the Table 2, so the repetitiousdetails will not be given here.

The Second Embodiment (Embodiment 2)

Please refer to FIG. 2A, FIG. 2B and FIG. 2C, FIG. 2A is a schematicview of the optical image capturing system according to the secondembodiment of the present application, FIG. 2B is longitudinal sphericalaberration curves, astigmatic field curves, and an optical distortioncurve of the optical image capturing system in the order from left toright according to the second embodiment of the present application, andFIG. 2C is a lateral aberration diagram of tangential fan, sagittal fan,the longest operation wavelength and the shortest operation wavelengthpassing through an edge of the entrance pupil and incident on the imageplane by 0.7 HOI according to the second embodiment of the presentapplication. As shown in FIG. 2A, in order from an object side to animage side, the optical image capturing system includes an aperture stop200, a first lens element 210, a second lens element 220, a third lenselement 230, a fourth lens element 240, a fifth lens element 250, asixth lens element 260, an IR-bandstop filter 280, an image plane 290,and an image sensing device 292.

The first lens element 210 has positive refractive power and it is madeof plastic material. The first lens element 210 has a convex object-sidesurface 212 and a concave image-side surface 214, and both of theobject-side surface 212 and the image-side surface 214 are aspheric andhave one inflection point.

The second lens element 220 has negative refractive power and it is madeof plastic material. The second lens element 220 has a convexobject-side surface 222 and a concave image-side surface 224, and bothof the object-side surface 222 and the image-side surface 224 areaspheric and have one inflection point.

The third lens element 230 has positive refractive power and it is madeof plastic material. The third lens element 230 has a convex object-sidesurface 232 and a concave image-side surface 234, and both of theobject-side surface 232 and the image-side surface 234 are aspheric andhave one inflection point.

The fourth lens element 240 has positive refractive power and it is madeof plastic material. The fourth lens element 240 has a concaveobject-side surface 242 and a convex image-side surface 244, and both ofthe object-side surface 242 and the image-side surface 244 are asphericand have one inflection point.

The fifth lens element 250 has positive refractive power and it is madeof plastic material. The fifth lens element 250 has a convex object-sidesurface 252 and a convex image-side surface 254, and both of theobject-side surface 252 and the image-side surface 254 are aspheric. Theobject-side surface 252 has an inflection point and the image-sidesurface 254 has two inflection points.

The sixth lens element 260 has negative refractive power and it is madeof plastic material. The sixth lens element 260 has a convex object-sidesurface 262 and a concave image-side surface 264. The object-sidesurface 262 and the image-side surface 264 both have an inflectionpoint. Hereby, the back focal length is reduced to miniaturize the lenselement effectively. In addition, the angle of incident with incominglight from an off-axis view field can be suppressed effectively and theaberration in the off-axis view field can be corrected further.

The IR-bandstop filter 280 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 260 and the image plane 290.

In the optical image capturing system of the second embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relation is satisfied: ΣPP=29.423 mm andf1/ΣPP=0.309. Hereby, it is favorable for allocating the positiverefractive power of a single lens element to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the second embodiment, a sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relation is satisfied: ΣNP=−12.565 mm andf2/ΣNP=0.783. Hereby, it is favorable for allocating the negativerefractive power of a single lens element to other negative lenselements.

Please refer to the following Table 3 and Table 4.

The detailed data of the optical image capturing system of the secondembodiment is as shown in Table 3.

TABLE 3 Data of the optical image capturing system f = 5.643 mm; f/HEP =2.0; HAF = 45 deg Focal Surface # Curvature Radius Thickness MaterialIndex Abbe # length 0 Object Plano At infinity 1 Ape. stop Plano −0.0582 Lens 1 3.658324313 0.602 Plastic 1.544 55.96 8.323 3 17.63357123 0.0004 Plano 0.181 5 Lens 2 5.291112924 0.300 Plastic 1.642 22.46 −10.239 62.877343151 0.230 7 Lens 3 4.705792136 0.629 Plastic 1.544 55.96 5.524 8−8.013181983 0.425 9 Lens 4 −1.629819063 0.890 Plastic 1.544 55.96 3.25110 −1.013835306 0.050 11 Lens 5 8.479879813 0.388 Plastic 1.642 22.463.773 12 −3.370625353 0.050 13 Lens 6 −78.90394352 0.400 Plastic 1.64222.46 −1.721 14 1.132857871 0.636 15 IR-bandstop Plano 0.420 BK_7 1.51764.13 filter 16 Plano 1.030 17 Image plane Plano 0.000 Referencewavelength (d-line) = 555 nmAs for the parameters of the aspheric surfaces of the second embodiment,reference is made to Table 4.

TABLE 4 Aspheric Coefficients Surface # 2 3 5 6 7 8 9 k −1.963561E+01−9.000000E+01 −5.827763E+01 −2.223771E+01 −2.057987E+01 −6.868330E+01−2.277878E+00 A4 5.993907E−02 −7.310861E−02 −1.000887E−01 −3.418683E−02−5.168499E−02 −7.679137E−02 −1.209867E−01 A6 −7.859196E−02 1.409351E−011.188257E−01 2.509797E−02 3.868551E−02 4.530778E−02 1.688018E−01 A8−3.642102E−03 −3.647496E−01 −2.359148E−01 −3.628928E−02 −6.406071E−02−5.325148E−02 −2.059202E−01 A10 3.691921E−01 5.009080E−01 2.250026E−012.315451E−02 5.923584E−02 3.034496E−02 1.682017E−01 A12 −8.862091E−01−4.298907E−01 −1.154022E−01 −1.404199E−02 −3.647943E−02 −6.110349E−03−7.096130E−02 A14 9.682616E−01 1.956535E−01 1.318927E−03 4.034643E−031.228726E−02 −2.253489E−04 1.442259E−02 A16 −5.219954E−01 −3.656746E−021.192381E−02 −2.490608E−04 −1.583653E−03 1.696937E−04 −1.123510E−03 A181.112092E−01 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A20 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 Surface # 10 11 1213 14 k −1.096038E−01 −2.457226E−01 −1.414328E−01 −4.890481E+00−1.285742E+00 A4 −2.147220E−01 −2.371507E−01 −7.486442E−02 −3.129158E−02−5.458921E−02 A6 2.126566E−01 2.425273E−01 5.518559E−02 7.201426E−031.088385E−02 A8 −1.066437E−01 −1.425446E−01 −2.595232E−02 −1.253499E−03−1.535375E−03 A10 3.059359E−02 5.529110E−02 9.763182E−03 1.391165E−041.404926E−04 A12 −4.225953E−03 −1.273438E−02 −2.050258E−03 −9.047444E−06−7.914381E−06 A14 1.626831E−04 1.565544E−03 2.106285E−04 3.204900E−072.470624E−07 A16 1.033356E−05 −7.966336E−05 −8.377410E−06 −4.889580E−09−3.260760E−09

In the second embodiment, the presentation of the aspheric surfaceformula is similar to that in the first embodiment. Besides, thedefinitions of parameters in following tables are equal to those in thefirst embodiment, so the repetitious details will not be given here.

The following contents may be deduced from Table 3 and Table 4.

Second embodiment (Primary reference wavelength = 555 nm) | f/f1 | |f/f2 | | f/f3 | | f/f4 | | f/f5 | | f/f6 | 0.62030 0.57389 0.611731.29335 0.83738 2.06508 Σ PPR Σ NPR Σ PPR/| Σ NPR | IN12/f IN56/fTP4/(IN34 + TP4 + IN45) 3.36275 2.63897 1.27427 0.06692 0.00886 0.47591| f1/f2 | | f2/f3 | (TP1 + IN12)/TP2 (TP6 + IN56)/TP5 0.92519 1.065943.61993 0.87134 HOS InTL HOS/HOI InS/HOS ODT % TDT % 8.40144 5.603902.10036 0.97841 1.29999 0.11016 HVT51 HVT52 HVT61 HVT62 HVT62/HOIHVT62/HOS 2.0737 0.51628 2.89885 3.09239 0.77310 0.36808 TP2/TP3 TP3/TP4InRS61 InRS62 | InRS61 |/TP6 | InRS62 |/TP6 0.38889 1.05811 0.350770.75500 0.87693 1.88751 PLTA PSTA NLTA NSTA SLTA SSTA −0.011 mm −0.022mm −0.011 mm −0.019 mm 0.004 mm −0.003 mm

The numerical related to the length of outline curve is shown accordingto table 3 and table 4.

Second embodiment (Reference wavelength = 555 nm) ARE ARE − 2(ARE/ ARE/ARE 1/2(HEP) value 1/2(HEP) HEP) % TP TP (%) 11 0.988 0.998 0.00957100.97% 0.602 165.61% 12 0.988 0.991 0.00304 100.31% 0.602 164.53% 210.988 0.992 0.00435 100.44% 0.300 330.83% 22 0.988 0.992 0.00435 100.44%0.300 330.83% 31 0.988 0.989 0.00127 100.13% 0.629 157.19% 32 0.9880.998 0.00940 100.95% 0.629 158.48% 41 0.988 1.052 0.06415 106.49% 0.890118.21% 42 0.988 1.099 0.11073 111.21% 0.890 123.44% 51 0.988 0.9880.00021 100.02% 0.388 254.46% 52 0.988 0.990 0.00185 100.19% 0.388254.88% 61 0.988 0.991 0.00245 100.25% 0.400 247.65% 62 0.988 1.0300.04161 104.21% 0.400 257.44% ARS ARS − (ARS/ ARS/ ARS EHD value EHDEHD) % TP TP (%) 11 1.070 1.081 0.010 100.97% 0.602 179.39% 12 1.2081.248 0.040 103.32% 0.602 207.11% 21 1.234 1.308 0.074 106.00% 0.300436.14% 22 1.468 1.504 0.036 102.43% 0.300 501.21% 31 1.567 1.582 0.015100.94% 0.629 251.33% 32 1.665 1.731 0.066 103.94% 0.629 275.02% 411.766 1.896 0.130 107.34% 0.890 213.00% 42 1.879 2.200 0.322 117.13%0.890 247.18% 51 2.269 2.355 0.085 103.75% 0.388 606.20% 52 2.763 2.7750.012 100.44% 0.388 714.54% 61 3.035 3.053 0.018 100.60% 0.400 763.33%62 3.265 3.454 0.189 105.78% 0.400 863.57%

The following contents may be deduced from Table 3 and Table 4.

Related inflection point values of second embodiment (Primary referencewavelength: 555 nm) HIF111 1.1617 HIF111/HOI 0.2904 SGI111 0.1414|SGI111|/(|SGI111| + TP1) 0.1372 HIF121 0.3353 HIF121/HOI 0.0838 SGI1210.0012 |SGI121|/(|SGI121| + TP1) 0.0013 HIF211 0.4791 HIF211/HOI 0.1198SGI211 0.0129 |SGI211|/(|SGI211| + TP2) 0.0355 HIF221 0.7576 HIF221/HOI0.1894 SGI221 0.0679 |SGI221|/(|SGI221| + TP2) 0.1625 HIF311 0.8241HIF311/HOI 0.2060 SGI311 0.0568 |SGI311|/(|SGI311| + TP3) 0.0594 HIF3210.1839 HIF321/HOI 0.0460 SGI321 0.0001 |SGI321|/(|SGI321| + TP3) 0.0001HIF411 1.8083 HIF411/HOI 0.4521 SGI411 −0.8709 |SGI411|/(|SGI411| + TP4)0.5059 HIF421 1.8683 HIF421/HOI 0.4671 SGI421 −1.1972|SGI421|/(|SGI421| + TP4) 0.5846 HIF511 1.4404 HIF511/HOI 0.3601 SGI5110.1668 |SGI511|/(|SGI511| + TP5) 0.2441 HIF521 0.2900 HIF521/HOI 0.0725SGI521 −0.0018 |SGI521|/(|SGI521| + TP5) 0.0034 HIF522 1.5844 HIF522/HOI0.3961 SGI522 0.1015 |SGI522|/(|SGI522| + TP5) 0.1642 HIF611 1.3703HIF611/HOI 0.3426 SGI611 0.1637 |SGI611|/(|SGI611| + TP6) 0.2904 HIF6211.0434 HIF621/HOI 0.2609 SGI621 0.2867 |SGI621|/(|SGI621| + TP6) 0.4175

The Third Embodiment (Embodiment 3)

Please refer to FIG. 3A, FIG. 3B and FIG. 3C, FIG. 3A is a schematicview of the optical image capturing system according to the thirdembodiment of the present application, FIG. 3B is longitudinal sphericalaberration curves, astigmatic field curves, and an optical distortioncurve of the optical image capturing system in the order from left toright according to the third embodiment of the present application, andFIG. 3C is a lateral aberration diagram of tangential fan, sagittal fan,the longest operation wavelength and the shortest operation wavelengthpassing through an edge of the entrance pupil and incident on the imageplane by 0.7 HOI according to the third embodiment of the presentapplication. As shown in FIG. 3A, in order from an object side to animage side, the optical image capturing system includes an aperture stop300, a first lens element 310, a second lens element 320, a third lenselement 330, a fourth lens element 340, a fifth lens element 350, asixth lens element 360, an IR-bandstop filter 380, an image plane 390,and an image sensing device 392.

The first lens element 310 has positive refractive power and it is madeof plastic material. The first lens element 310 has a convex object-sidesurface 312 and a concave image-side surface 314, and both of theobject-side surface 312 and the image-side surface 314 are aspheric andboth have one inflection point.

The second lens element 320 has negative refractive power and it is madeof plastic material. The second lens element 320 has a convexobject-side surface 322 and a concave image-side surface 324, and bothof the object-side surface 322 and the image-side surface 324 areaspheric. The object-side surface 322 has an inflection and theimage-side surface 324 has two inflection points.

The third lens element 330 has positive refractive power and it is madeof plastic material. The third lens element 330 has a convex object-sidesurface 332 and a convex image-side surface 334, and both of theobject-side surface 332 and the image-side surface 334 are aspheric. Theobject-side surface 332 has two inflection points and the image-sidesurface 334 has one inflection point.

The fourth lens element 340 has positive refractive power and it is madeof plastic material. The fourth lens element 340 has a concaveobject-side surface 342 and a convex image-side surface 344, and both ofthe object-side surface 342 and the image-side surface 344 are asphericand both have one inflection point.

The fifth lens element 350 has positive refractive power and it is madeof plastic material. The fifth lens element 350 has a convex object-sidesurface 352 and a convex image-side surface 354, and both of theobject-side surface 352 and the image-side surface 354 are aspheric. Theobject-side surface 352 has three inflection points and the image-sidesurface 354 has two inflection points.

The sixth lens element 360 has negative refractive power and it is madeof plastic material. The sixth lens element 360 has a concaveobject-side surface 362 and a concave image-side surface 364. Theobject-side surface 362 has three inflection points and the image-sidesurface 364 has one inflection point. Hereby, the back focal length isreduced to miniaturize the lens element effectively. In addition, theangle of incident with incoming light from an off-axis view field can besuppressed effectively and the aberration in the off-axis view field canbe corrected further.

The IR-bandstop filter 380 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 360 and the image plane 390.

In the optical image capturing system of the third embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relation is satisfied: ΣPP=20.647 mm andf1/ΣPP=0.378. Hereby, it is favorable for allocating the positiverefractive power of a single lens element to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the third embodiment, a sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relation is satisfied: ΣNP=−11.437 mm andf2/ΣNP=0.851. Hereby, it is favorable for allocating the negativerefractive power of a single lens element to other negative lenselements.

Please refer to the following Table 5 and Table 6.

The detailed data of the optical image capturing system of the thirdembodiment is as shown in Table 5.

TABLE 5 Data of the optical image capturing system f = 3.953 mm; f/HEP =2.1; HAF = 45 deg Focal Surface# Curvature Radius Thickness MaterialIndex Abbe # length 0 Object Plano At infinity 1 Ape. stop Plano −0.0252 Lens 1 3.81542436 0.600 Plastic 1.544 55.96 7.799 3 34.50280757 0.0004 1E+18 0.177 5 Lens 2 6.321748832 0.300 Plastic 1.642 22.46 −9.731 63.097121294 0.230 7 Lens 3 4.689857455 0.632 Plastic 1.544 55.96 5.871 8−9.663099713 0.421 9 Lens 4 −1.661206776 0.900 Plastic 1.544 55.96 3.07310 −0.99472581 0.050 11 Lens 5 8.954465809 0.383 Plastic 1.642 22.463.904 12 −3.463604208 0.050 13 Lens 6 −1288.388647 0.400 Plastic 1.64222.46 −1.706 14 1.106045615 0.648 15 IR-bandstop Plano 0.420 BK_7 1.51764.13 filter 16 Plano 1.030 17 Image plane Plano 0.000 Referencewavelength (d-line) = 555 nmAs for the parameters of the aspheric surfaces of the third embodiment,reference is made to Table 6.

TABLE 6 Aspheric Coefficients Surface # 2 3 5 6 7 8 9 k −1.859569E+01−9.000000E+01 −5.827763E+01 −2.201045E+01 −3.071565E+01 −6.868330E+01−2.240268E+00 A4 5.397186E−02 −6.874496E−02 −1.044717E−01 −4.674811E−02−4.788171E−02 −6.975970E−02 −1.094048E−01 A6 −1.029929E−01 1.292817E−011.546611E−01 6.431470E−02 2.656855E−02 2.708669E−02 1.554384E−01 A81.157681E−01 −3.776106E−01 −3.548482E−01 −1.088303E−01 −5.533747E−02−3.181018E−02 −2.041498E−01 A10 9.381219E−02 5.379544E−01 4.135343E−019.508887E−02 5.527797E−02 9.933762E−03 1.739659E−01 A12 −5.561517E−01−4.770660E−01 −2.959291E−01 −5.662340E−02 −3.669403E−02 6.653198E−03−7.519769E−02 A14 7.679582E−01 2.266518E−01 9.389031E−02 1.824209E−021.327483E−02 −4.496588E−03 1.554354E−02 A16 −4.744245E−01 −4.473772E−02−6.632552E−03 −2.220511E−03 −1.805507E−03 7.317763E−04 −1.225014E−03 A181.112092E−01 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A20 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 Surface # 10 11 1213 14 k −2.010374E+00 −1.333877E+01 −9.000000E+01 −8.999932E+01−5.643945E+00 A4 −6.043545E−02 −9.543444E−02 −3.367125E−02 1.008296E−015.893671E−03 A6 7.567328E−02 8.483173E−02 6.945227E−02 −5.300271E−02−1.025863E−02 A8 −8.829741E−02 −3.554425E−02 −3.327932E−02 1.322364E−023.031928E−03 A10 5.818714E−02 8.653885E−03 7.762124E−03 −1.774737E−03−5.199253E−04 A12 −1.918167E−02 −1.534608E−03 −9.931372E−04 1.205295E−045.578526E−05 A14 3.047731E−03 1.910173E−04 6.721175E−05 −3.102724E−06−3.488861E−06 A16 −1.827837E−04 −1.135710E−05 −1.891201E−06−1.158597E−08 9.462409E−08 A18 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A20 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00

The presentation of the aspheric surface formula in the third embodimentis similar to that in the first embodiment. Besides, the definitions ofparameters in following tables are equal to those in the firstembodiment so the repetitious details will not be given here.

The following contents may be deduced from Table 5 and Table 6.

The numerical related to the length of outline curve is shown accordingto table 5 and table 6.

Third embodiment (Reference wavelength = 555 nm) ARE ARE − 2(ARE/ ARE/ARE 1/2(HEP) value 1/2(HEP) HEP) % TP TP (%) 11 0.941 0.948 0.00740100.79% 0.600 158.11% 12 0.941 0.944 0.00298 100.32% 0.600 157.37% 210.941 0.944 0.00283 100.30% 0.300 314.64% 22 0.941 0.945 0.00364 100.39%0.300 314.91% 31 0.941 0.942 0.00108 100.12% 0.632 149.17% 32 0.9410.948 0.00690 100.73% 0.632 150.09% 41 0.941 0.995 0.05431 105.77% 0.900110.60% 42 0.941 1.041 0.10011 110.64% 0.900 115.69% 51 0.941 0.9410.00005 100.01% 0.383 245.79% 52 0.941 0.943 0.00233 100.25% 0.383246.39% 61 0.941 0.943 0.00242 100.26% 0.400 235.87% 62 0.941 0.9820.04045 104.30% 0.400 245.38% ARS ARS − (ARS/ ARS/ ARS EHD value EHDEHD) % TP TP (%) 11 1.040 1.047 0.007 100.72% 0.600 174.59% 12 1.1841.227 0.043 103.67% 0.600 204.55% 21 1.217 1.286 0.069 105.66% 0.300428.53% 22 1.453 1.483 0.030 102.04% 0.300 494.36% 31 1.555 1.571 0.017101.09% 0.632 248.81% 32 1.652 1.729 0.076 104.63% 0.632 273.73% 411.757 1.890 0.132 107.52% 0.900 209.95% 42 1.873 2.204 0.331 117.65%0.900 244.88% 51 2.258 2.337 0.079 103.50% 0.383 610.39% 52 2.752 2.7670.015 100.55% 0.383 722.73% 61 3.004 3.024 0.021 100.69% 0.400 756.10%62 3.244 3.448 0.204 106.28% 0.400 861.96%

The following contents may be deduced from Table 5 and Table 6.

Related inflection point values of third embodiment (Primary referencewavelength: 555 nm) HIF111 0.8288 HIF111/HOI 0.2072 SGI111 0.0860|SGI111|/(|SGI111| + TP1) 0.1254 HIF121 0.2033 HIF121/HOI 0.0508 SGI1210.0005 |SGI121|/(|SGI121| + TP1) 0.0008 HIF211 0.3653 HIF211/HOI 0.0913SGI211 0.0085 |SGI211|/(|SGI211| + TP2) 0.0276 HIF221 0.6049 HIF221/HOI0.1512 SGI221 0.0459 |SGI221|/(|SGI221| + TP2) 0.1326 HIF222 1.4188HIF222/HOI 0.3547 SGI222 −0.0363 |SGI222|/(|SGI222| + TP2) 0.1079 HIF3110.5145 HIF311/HOI 0.1286 SGI311 0.0230 |SGI311|/(|SGI311| + TP3) 0.0351HIF312 1.3524 HIF312/HOI 0.3381 SGI312 −0.0401 |SGI312|/(|SGI312| + TP3)0.0597 HIF321 1.4491 HIF321/HOI 0.3623 SGI321 −0.3162|SGI321|/(|SGI321| + TP3) 0.3336 HIF411 1.0420 HIF411/HOI 0.2605 SGI411−0.3436 |SGI411|/(|SGI411| + TP4) 0.2763 HIF421 1.2456 HIF421/HOI 0.3114SGI421 −0.6573 |SGI421|/(|SGI421| + TP4) 0.4221 HIF511 0.3568 HIF511/HOI0.0892 SGI511 0.0057 |SGI511|/(|SGI511| + TP5) 0.0146 HIF512 0.8081HIF512/HOI 0.2020 SGI512 0.0130 |SGI512|/(|SGI512| + TP5) 0.0328 HIF5131.3537 HIF513/HOI 0.3384 SGI513 0.0292 |SGI513|/(|SGI513| + TP5) 0.0709HIF521 0.5897 HIF521/HOI 0.1474 SGI521 −0.0363 |SGI521|/(|SGI521| + TP5)0.0866 HIF522 1.6383 HIF522/HOI 0.4096 SGI522 0.0064|SGI522|/(|SGI522| + TP5) 0.0166 HIF611 0.0253 HIF611/HOI 0.0063 SGI611−0.0000 |SGI611|/(|SGI611| + TP6) 0.0000 HIF612 1.2750 HIF612/HOI 0.3187SGI612 0.1125 |SGI612|/(|SGI612| + TP6) 0.2194 HIF613 2.7416 HIF613/HOI0.6854 SGI613 0.2270 |SGI613|/(|SGI613| + TP6) 0.3620 HIF621 0.9638HIF621/HOI 0.2409 SGI621 0.2673 |SGI621|/(|SGI621| + TP6) 0.4006

The Fourth Embodiment (Embodiment 4)

Please refer to FIG. 4A, FIG. 4B and FIG. 4C, FIG. 4A is a schematicview of the optical image capturing system according to the fourthembodiment of the present application, FIG. 4B is longitudinal sphericalaberration curves, astigmatic field curves, and an optical distortioncurve of the optical image capturing system in the order from left toright according to the fourth embodiment of the present application, andFIG. 4C is a lateral aberration diagram of tangential fan, sagittal fan,the longest operation wavelength and the shortest operation wavelengthpassing through an edge of the entrance pupil and incident on the imageplane by 0.7 HOI according to the fourth embodiment of the presentapplication. As shown in FIG. 4A, in order from an object side to animage side, the optical image capturing system includes a first lenselement 410, an aperture stop 400, a second lens element 420, a thirdlens element 430, a fourth lens element 440, a fifth lens element 450, asixth lens element 460, an IR-bandstop filter 480, an image plane 490,and an image sensing device 492.

The first lens element 410 has positive refractive power and it is madeof plastic material. The first lens element 410 has a convex object-sidesurface 412 and a concave image-side surface 414, and both of theobject-side surface 412 and the image-side surface 414 are aspheric andhave one inflection point.

The second lens element 420 has negative refractive power and it is madeof plastic material. The second lens element 420 has a convexobject-side surface 422 and a concave image-side surface 424, and bothof the object-side surface 422 and the image-side surface 424 areaspheric and have one inflection point.

The third lens element 430 has positive refractive power and it is madeof plastic material. The third lens element 430 has a convex object-sidesurface 432 and a convex image-side surface 434, and both of theobject-side surface 432 and the image-side surface 434 are aspheric. Theobject-side surface 432 has two inflection points and the image-sidesurface 434 and has one inflection point.

The fourth lens element 440 has positive refractive power and it is madeof plastic material. The fourth lens element 440 has a concaveobject-side surface 442 and a convex image-side surface 444, and both ofthe object-side surface 442 and the image-side surface 444 are asphericand have one inflection point.

The fifth lens element 450 has positive refractive power and it is madeof plastic material. The fifth lens element 450 has a convex object-sidesurface 452 and a convex image-side surface 454, and both of theobject-side surface 452 and the image-side surface 454 are aspheric. Theobject-side surface 452 has three inflection points and the image-sidesurface 454 and has two inflection points.

The sixth lens element 460 has negative refractive power and it is madeof plastic material. The sixth lens element 460 has a convex object-sidesurface 462 and a concave image-side surface 464. The object-sidesurface 462 has two inflection points and the image-side surface 464 hasan inflection point. Hereby, the back focal length is reduced tominiaturize the lens element effectively. In addition, the angle ofincident with incoming light from an off-axis view field can besuppressed effectively and the aberration in the off-axis view field canbe corrected further.

The IR-bandstop filter 480 is made of plastic material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 460 and the image plane 490.

In the optical image capturing system of the fourth embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relation is satisfied: ΣPP=20.463 mm andf1/ΣPP=0.368. Hereby, it is favorable for allocating the positiverefractive power of a single lens element to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the fourth embodiment, a sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relation is satisfied: ΣNP=−11.127 mm andf2/ΣNP=0.849. Hereby, it is favorable for allocating the negativerefractive power of a single lens element to other negative lenselements.

Please refer to the following Table 7 and Table 8.

The detailed data of the optical image capturing system of the fourthembodiment is as shown in Table 7.

TABLE 7 Data of the optical image capturing system f = 3.953 mm; f/HEP =2.2; HAF = 45 deg Focal Surface# Curvature Radius Thickness MaterialIndex Abbe # length 0 Object Plano At infinity 1 Ape. Plano −0.011 stop2 Lens 1 3.874273002 0.578 Plastic 1.544 55.96 7.534 3 62.55736428 0.0004 1E+18 0.180 5 Lens 2 7.075906865 0.300 Plastic 1.642 22.46 −9.445 63.226004031 0.239 7 Lens 3 4.603635743 0.637 Plastic 1.544 55.96 6.037 8−11.05896415 0.422 9 Lens 4 −1.67306319 0.900 Plastic 1.544 55.96 3.05710 −0.99456257 0.050 11 Lens 5 8.50550655 0.380 Plastic 1.642 22.463.835 12 −3.446458513 0.050 13 Lens 6 288.1612039 0.400 Plastic 1.64222.46 −1.682 14 r 1.084819191 0.648 15 IR-band Plano 0.420 BK_7 1.51764.13 stop filter 16 Plano 1.030 17 Image Plano plane Referencewavelength(d-line) = 555 nmAs for the parameters of the aspheric surfaces of the fourth embodiment,reference is made to Table 8.

TABLE 8 Aspheric Coefficients Surface # 2 3 5 6 7 8 9 k −1.975031E+01−9.000000E+01 −5.827750E+01 −2.231523E+01 −3.999062E+01 −6.868028E+01−2.232173E+00 A4 6.566516E−02 −6.541466E−02 −1.108596E−01 −5.345374E−02−3.858182E−02 −6.496371E−02 −1.016826E−01 A6 −2.160242E−01 1.044811E−011.805143E−01 7.380626E−02 1.558833E−02 1.655399E−02 1.404297E−01 A85.787925E−01 −3.290994E−01 −4.654192E−01 −1.188230E−01 −5.990319E−02−1.538121E−02 −1.898174E−01 A10 −9.467813E−01 4.798303E−01 6.683454E−011.005382E−01 7.753432E−02 −7.532199E−03 1.674289E−01 A12 7.269769E−01−4.594323E−01 −6.279983E−01 −6.155161E−02 −5.984151E−02 1.853751E−02−7.386623E−02 A14 −5.113311E−02 2.458585E−01 3.142260E−01 2.248675E−022.320012E−02 −9.033276E−03 1.540271E−02 A16 −2.644827E−01 −5.674044E−02−6.339533E−02 −3.369276E−03 −3.305778E−03 1.414097E−03 −1.210635E−03 A181.112092E−01 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A20 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 Surface # 10 11 1213 14 k −1.992574E+00 −1.333945E+01 −9.000000E+01 −8.999932E+01−5.556987E+00 A4 −6.003930E−02 −9.994773E−02 −2.724956E−02 1.053005E−016.039990E−03 A6 7.282356E−02 8.801968E−02 6.341556E−02 −5.858546E−02−1.116170E−02 A8 −8.593294E−02 −3.645659E−02 −3.078908E−02 1.562830E−023.422519E−03 A10 5.740882E−02 8.563675E−03 7.199098E−03 −2.290731E−03−5.953725E−04 A12 −1.908186E−02 −1.428716E−03 −9.197079E−04 1.790568E−046.346665E−05 A14 3.047681E−03 1.702580E−04 6.200950E−05 −6.437461E−06−3.905286E−06 A16 −1.832913E−04 −1.001851E−05 −1.735507E−06 6.299563E−081.042365E−07 A18 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 A20 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00

The presentation of the aspheric surface formula in the fourthembodiment is similar to that in the first embodiment. Besides thedefinitions of parameters in following tables are equal to those in thefirst embodiment so the repetitious details will not be given here.

The following contents may be deduced from Table 7 and Table 8.

Fourth embodiment (Primary reference wavelength: 555 nm) |f/f1| |f/f2||f/f3| |f/f4| |f/f5| |f/f6| 0.52462 0.41850 0.65472 1.29302 1.030652.34949 TP4/(IN34 + Σ PPR Σ NPR Σ PPR/|Σ NPR| IN12/f IN56/f TP4 + IN45)3.50301 2.76799 1.26554 0.04545 0.01265 0.65601 |f1/f2| |f2/f3| (TP1 +IN12)/TP2 (TP6 + IN56)/TP5 0.79773 1.56444 2.52431 1.18367 HOS InTLHOS/HOI InS/HOS ODT % TDT % 6.23267 4.13501 1.55817 0.99816 1.598500.71821 HVT51 HVT52 HVT61 HVT62 HVT62/HOI HVT62/HOS 1.57405 1.032422.34081 2.27234 0.56809 0.36459 TP2/ TP3 TP3/TP4 InRS61 InRS62|InRS61|/TP6 |InRS62|/TP6 0.47118 0.70745 0.20057 0.24225 0.501430.60564 PLTA PSTA NLTA NSTA SLTA SSTA 0.003 mm −0.011 −0.007 mm −0.011mm 0.008 mm 0.002 mm mm

The numerical related to the length of outline curve is shown accordingto table 7 and table 8.

Fourth embodiment (Reference wavelength = 555 nm) ARE ARE − 2(ARE/HEP)ARE/TP ARE ½(HEP) value ½(HEP) % TP (%) 11 0.898 0.904 0.00597 100.66%0.578 156.54% 12 0.898 0.901 0.00225 100.25% 0.578 155.90% 21 0.8980.900 0.00157 100.18% 0.300 299.96% 22 0.898 0.901 0.00288 100.32% 0.300300.40% 31 0.898 0.899 0.00083 100.09% 0.637 141.22% 32 0.898 0.9030.00462 100.51% 0.637 141.81% 41 0.898 0.945 0.04647 105.17% 0.900104.98% 42 0.898 0.988 0.08946 109.96% 0.900 109.75% 51 0.898 0.898−0.00017  99.98% 0.380 236.24% 52 0.898 0.900 0.00191 100.21% 0.380236.79% 61 0.898 0.900 0.00187 100.21% 0.400 225.04% 62 0.898 0.9360.03793 104.22% 0.400 234.06% ARS (ARS/EHD) ARS/TP ARS EHD value ARS −EHD % TP (%) 11 0.999 1.006 0.007 100.66% 0.578 174.17% 12 1.143 1.1820.039 103.38% 0.578 204.65% 21 1.181 1.239 0.058 104.93% 0.300 413.15%22 1.427 1.452 0.025 101.76% 0.300 483.89% 31 1.523 1.543 0.020 101.31%0.637 242.38% 32 1.628 1.715 0.087 105.35% 0.637 269.40% 41 1.739 1.8730.133 107.66% 0.900 208.06% 42 1.863 2.196 0.334 117.92% 0.900 244.05%51 2.249 2.319 0.070 103.11% 0.380 609.92% 52 2.723 2.738 0.014 100.53%0.380 720.09% 61 2.952 2.973 0.021 100.72% 0.400 743.22% 62 3.212 3.4260.215 106.68% 0.400 856.58%

The following contents may be deduced from Table 7 and Table 8.

Related inflection point values of fourth embodiment (Primary referencewavelength: 555 nm) HIF111 0.7935 HIF111/HOI 0.1984 SGI111 0.0774|SGI111|/(|SGI111| + TP1) 0.1182 HIF121 0.1485 HIF121/HOI 0.0371 SGI1210.0001 |SGI121|/(|SGI121| + TP1) 0.0003 HIF211 0.3470 HIF211/HOI 0.0868SGI211 0.0069 |SGI211|/(|SGI211| + TP2) 0.0224 HIF221 0.5908 HIF221/HOI0.1477 SGI221 0.0421 |SGI221|/(|SGI221| + TP2) 0.1232 HIF311 0.5060HIF311/HOI 0.1265 SGI311 0.0227 |SGI311|/(|SGI311| + TP3) 0.0344 HIF3121.3312 HIF312/HOI 0.3328 SGI312 −0.0460 |SGI312|/(|SGI312| + TP3) 0.0674HIF321 1.4847 HIF321/HOI 0.3712 SGI321 −0.3430 |SGI321|/(|SGI321| + TP3)0.3501 HIF411 1.0400 HIF411/HOI 0.2600 SGI411 −0.3389|SGI411|/(|SGI411| + TP4) 0.2736 HIF421 1.2450 HIF421/HOI 0.3113 SGI421−0.6604 |SGI421|/(|SGI421| + TP4) 0.4232 HIF511 0.3567 HIF511/HOI 0.0892SGI511 0.0060 |SGI511|/(|SGI511| + TP5) 0.0155 HIF512 0.8181 HIF512/HOI0.2045 SGI512 0.0136 |SGI512|/(|SGI512| + TP5) 0.0346 HIF513 1.3437HIF513/HOI 0.3359 SGI513 0.0282 |SGI513|/(|SGI513| + TP5) 0.0690 HIF5210.5750 HIF521/HOI 0.1437 SGI521 −0.0345 |SGI521|/(|SGI521| + TP5) 0.0832HIF522 1.6402 HIF522/HOI 0.4100 SGI522 0.0097 |SGI522|/(|SGI522| + TP5)0.0248 HIF611 1.2501 HIF611/HOI 0.3125 SGI611 0.1106|SGI611|/(|SGI611| + TP6) 0.2166 HIF612 2.7225 HIF612/HOI 0.6806 SGI6120.2174 |SGI612|/(|SGI612| + TP6) 0.3521 HIF621 0.9491 HIF621/HOI 0.2373SGI621 0.2649 |SGI621|/(|SGI621| + TP6) 0.3984

The Fifth Embodiment (Embodiment 5)

Please refer to FIG. 5A, FIG. 5B and FIG. 5C, FIG. 5A is a schematicview of the optical image capturing system according to the fifthembodiment of the present application, FIG. 5B is longitudinal sphericalaberration curves, astigmatic field curves, and an optical distortioncurve of the optical image capturing system in the order from left toright according to the fifth embodiment of the present application, andFIG. 5C is a lateral aberration diagram of tangential fan, sagittal fan,the longest operation wavelength and the shortest operation wavelengthpassing through an edge of the entrance pupil and incident on the imageplane by 0.7 HOI according to the fifth embodiment of the presentapplication. As shown in FIG. 5A, in order from an object side to animage side, the optical image capturing system includes an aperture stop500, a first lens element 510, a second lens element 520, a third lenselement 530, a fourth lens element 540, a fifth lens element 550, asixth lens element 560, an IR-bandstop filter 580, an image plane 590,and an image sensing device 592.

The first lens element 510 has positive refractive power and it is madeof plastic material. The first lens element 510 has a convex object-sidesurface 512 and a convex image-side surface 514, and both of theobject-side surface 512 and the image-side surface 514 are aspheric. Theimage-side surface 514 has one inflection point.

The second lens element 520 has negative refractive power and it is madeof plastic material. The second lens element 520 has a convexobject-side surface 522 and a concave image-side surface 524, and bothof the object-side surface 522 and the image-side surface 524 areaspheric. The image-side surface 524 has one inflection point.

The third lens element 530 has positive refractive power and it is madeof plastic material. The third lens element 530 has a convex object-sidesurface 532 and a concave image-side surface 534, and both of theobject-side surface 532 and the image-side surface 534 are aspheric andhave two inflection points.

The fourth lens element 540 has positive refractive power and it is madeof plastic material. The fourth lens element 540 has a concaveobject-side surface 542 and a convex image-side surface 544, and both ofthe object-side surface 542 and the image-side surface 544 are asphericand have one inflection point.

The fifth lens element 550 has positive refractive power and it is madeof plastic material. The fifth lens element 550 has a convex object-sidesurface 552 and a concave image-side surface 554, and both of theobject-side surface 552 and the image-side surface 554 are aspheric andhave two inflection points.

The sixth lens element 560 has negative refractive power and it is madeof plastic material. The sixth lens element 560 has a convex object-sidesurface 562 and a concave image-side surface 564. The object-sidesurface 562 has three inflection points and the image-side surface 564has one inflection point. Hereby, the back focal length is reduced tominiaturize the lens element effectively. In addition, the angle ofincident with incoming light from an off-axis view field can besuppressed effectively and the aberration in the off-axis view field canbe corrected further.

The IR-bandstop filter 580 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 560 and the image plane 590.

In the optical image capturing system of the fifth embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relation is satisfied: ΣPP=33.024 mm andf1/ΣPP=0.269. Hereby, it is favorable for allocating the positiverefractive power of a single lens element to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the fifth embodiment, a sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relation is satisfied: ΣNP=−12.331 mm andf2/ΣNP=0.735. Hereby, it is favorable for allocating the negativerefractive power of a single lens element to other negative lenselements.

Please refer to the following Table 9 and Table 10.

The detailed data of the optical image capturing system of the fifthembodiment is as shown in Table 9.

TABLE 9 Data of the optical image capturing system f = 4.718 mm; f/HEP =2.0; HAF = 40 deg Focal Surface # Curvature Radius Thickness MaterialIndex Abbe # length 0 Object Plano At infinity 1 Ape. stop Plano −0.0552 Lens 1 6.517943431 0.808 Plastic 1.544 55.96 8.872 3 −18.073222810.000 4 1E+18 0.223 5 Lens 2 5.973853205 0.350 Plastic 1.642 22.46−9.062 6 2.892257501 0.236 7 Lens 3 3.284674656 0.900 Plastic 1.54455.96 7.445 8 15.42528289 0.634 9 Lens 4 −2.057423518 0.900 Plastic1.544 55.96 3.853 10 −1.201138101 0.050 11 Lens 5 3.013859874 0.375Plastic 1.642 22.46 12.854 12 4.493353752 0.178 13 Lens 6 9.0829187010.453 Plastic 1.642 22.46 −3.269 14 1.683192517 0.678 15 IR-bandstopPlano 0.420 BK_7 1.517 64.13 filter 16 Plano 1.180 17 Image plane PlanoReference wavelength (d-line) = 555 nmAs for the parameters of the aspheric surfaces of the fifth embodiment,reference is made to Table 10.

TABLE 10 Aspheric Coefficients Surface # 2 3 5 6 7 8 9 k −3.474756E−01−8.999993E+01 3.777386E+00 −1.980901E+01 −2.619781E+01  −6.850519E+01−7.953836E−01 A4 −2.724251E−02 −4.215135E−02 −7.005564E−02  9.229578E−05 1.618652E−02 −1.875489E−02  1.030411E−02 A6  1.805377E−01 1.503110E−02 4.538811E−02 −3.568418E−03 −2.284271E−02   5.522315E−03−5.494204E−03 A8 −8.204402E−01 −4.223478E−02 −7.549720E−02 −1.497487E−02 7.142970E−03 −2.368744E−03  5.609844E−03 A10  1.859045E+00 3.931983E−02 6.675384E−02  1.546547E−02 9.495566E−04 −6.948804E−04−2.773061E−04 A12 −2.387640E+00 −1.881701E−02 −3.544233E−02 −8.351530E−03 −2.369685E−03   6.699414E−04 −1.061670E−03 A14 1.753068E+00  4.259879E−03 1.033496E−02  2.312216E−03 8.331559E−04−2.078561E−04  3.549910E−04 A16 −6.864993E−01 −3.321840E−04−1.249332E−03  −2.466164E−04 −8.753097E−05   2.290213E−05 −3.321804E−05A18  1.112092E−01  0.000000E+00 0.000000E+00  0.000000E+00 0.000000E+00 0.000000E+00  0.000000E+00 A20  0.000000E+00  0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00  0.000000E+00  0.000000E+00 Surface # 10 1112 13 14 k −2.668391E+00 −3.716500E−02 −1.380570E+01  −8.999813E+01 −4.793150E+00  A4 −6.444589E−02 −8.158345E−03 1.501687E−01 1.736128E−011.454380E−02 A6  2.990923E−02 −4.888527E−02 −1.750827E−01 −1.469938E−01  −1.773318E−02  A8 −1.712782E−02  2.843227E−028.067986E−02 5.399969E−02 5.507679E−03 A10  9.263761E−03 −7.631671E−03−1.970862E−02  −1.073442E−02  −8.857225E−04  A12 −3.147265E−03 1.027716E−03 2.683876E−03 1.206056E−03 7.984763E−05 A14  5.656657E−04−6.919892E−05 −1.935124E−04  −7.232048E−05  −3.840760E−06  A16−3.961599E−05  1.981548E−06 5.782850E−06 1.801333E−06 7.670776E−08 A18 0.000000E+00  0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A20 0.000000E+00  0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00

The presentation of the aspheric surface formula in the fifth embodimentis similar to that in the first embodiment. Besides the definitions ofparameters in following tables are equal to those in the firstembodiment so the repetitious details will not be given here.

The following contents may be deduced from Table 9 and Table 10.

The numerical related to the length of outline curve is shown accordingto table 9 and table 10.

Fifth embodiment (Reference wavelength = 555 nm) ARE ARE − 2(ARE/ ARE/ARE 1/2(HEP) value 1/2(HEP) HEP) % TP TP (%) 11 1.180 1.181 0.00172100.15% 0.808 146.14% 12 1.180 1.193 0.01311 101.11% 0.808 147.55% 211.180 1.181 0.00184 100.16% 0.350 337.53% 22 1.180 1.188 0.00809 100.69%0.350 339.32% 31 1.180 1.187 0.00772 100.65% 0.900 131.92% 32 1.1801.179 −0.00033 99.97% 0.900 131.02% 41 1.180 1.235 0.05529 104.69% 0.900137.20% 42 1.180 1.314 0.13479 111.43% 0.900 146.04% 51 1.180 1.1930.01319 101.12% 0.375 318.43% 52 1.180 1.194 0.01421 101.20% 0.375318.70% 61 1.180 1.193 0.01331 101.13% 0.453 263.39% 62 1.180 1.2250.04532 103.84% 0.453 270.46% ARS ARS − (ARS/ ARS/ ARS EHD value EHDEHD) % TP TP (%) 11 1.188 1.190 0.002 100.16% 0.808 147.26% 12 1.4201.469 0.049 103.46% 0.808 181.72% 21 1.540 1.575 0.035 102.27% 0.350450.09% 22 1.806 1.825 0.019 101.05% 0.350 521.51% 31 1.942 1.954 0.012100.62% 0.900 217.06% 32 2.055 2.157 0.101 104.93% 0.900 239.62% 412.080 2.252 0.172 108.27% 0.900 250.19% 42 2.155 2.555 0.400 118.58%0.900 283.88% 51 2.490 2.662 0.172 106.90% 0.375 710.74% 52 2.756 2.8300.074 102.68% 0.375 755.55% 61 2.997 3.027 0.030 101.01% 0.453 668.39%62 3.392 3.503 0.112 103.29% 0.453 773.60%

The following contents may be deduced from Table 9 and Table 10.

Related inflection point values of fifth embodiment (Primary referencewavelength: 555 nm) HIF111 0.7844 HIF111/HOI 0.1961 SGI111 0.0417 |SGI111 |/(| SGI111 | + TP1) 0.0490 HIF211 0.5069 HIF211/HOI 0.1267SGI211 0.0176 | SGI211 |/(| SGI211 | + TP2) 0.0478 HIF221 0.7612HIF221/HOI 0.1903 SGI221 0.0780 | SGI221 |/(| SGI221 | + TP2) 0.1822HIF311 0.8254 HIF311/HOI 0.2063 SGI311 0.0813 | SGI311 |/(| SGI311 | +TP3) 0.0828 HIF312 1.6612 HIF312/HOI 0.4153 SGI312 0.1092 | SGI312 |/(|SGI312 | + TP3) 0.1082 HIF321 0.5519 HIF321/HOI 0.1380 SGI321 0.0081 |SGI321 |/(| SGI321 | + TP3) 0.0089 HIF322 1.9412 HIF322/HOI 0.4853SGI322 −0.2695 | SGI322 |/(| SGI322 | + TP3) 0.2305 HIF411 1.6525HIF411/HOI 0.4131 SGI411 −0.5933 | SGI411 |/(| SGI411 | + TP4) 0.3973HIF421 1.6126 HIF421/HOI 0.4031 SGI421 −0.9139 | SGI421 |/(| SGI421 | +TP4) 0.5038 HIF511 0.8232 HIF511/HOI 0.2058 SGI511 0.1006 | SGI511 |/(|SGI511 | + TP5) 0.2117 HIF512 2.3785 HIF512/HOI 0.5946 SGI512 −0.1265 |SGI512 |/(| SGI512 | + TP5) 0.2524 HIF521 0.8339 HIF521/HOI 0.2085SGI521 0.1000 | SGI521 |/(| SGI521 | + TP5) 0.2107 HIF522 2.6546HIF522/HOI 0.6636 SGI522 −0.0369 | SGI522 |/(| SGI522 | + TP5) 0.0897HIF611 0.9491 HIF611/HOI 0.2373 SGI611 0.1045 | SGI611 |/(| SGI611 | +TP6) 0.1875 HIF612 1.7296 HIF612/HOI 0.4324 SGI612 0.2000 | SGI612 |/(|SGI612 | + TP6) 0.3064 HIF613 2.2172 HIF613/HOI 0.5543 SGI613 0.2236 |SGI613 |/(| SGI613 | + TP6) 0.3305 HIF621 1.0633 HIF621/HOI 0.2658SGI621 0.2603 | SGI621 |/(| SGI621 | + TP6) 0.3650

The Sixth Embodiment (Embodiment 6)

Please refer to FIG. 6A, FIG. 6B and FIG. 6C, FIG. 6A is a schematicview of the optical image capturing system according to the sixthEmbodiment of the present application, FIG. 6B is longitudinal sphericalaberration curves, astigmatic field curves, and an optical distortioncurve of the optical image capturing system in the order from left toright according to the sixth Embodiment of the present application, andFIG. 6C is a lateral aberration diagram of tangential fan, sagittal fan,the longest operation wavelength and the shortest operation wavelengthpassing through an edge of the entrance pupil and incident on the imageplane by 0.7 HOI according to the sixth embodiment of the presentapplication. As shown in FIG. 6A, in order from an object side to animage side, the optical image capturing system includes an aperture stop600, a first lens element 610, a second lens element 620, a third lenselement 630, a fourth lens element 640, a fifth lens element 650, asixth lens element 660, an IR-bandstop filter 680, an image plane 690,and an image sensing device 692.

The first lens element 610 has positive refractive power and it is madeof plastic material. The first lens element 610 has a convex object-sidesurface 612 and a convex image-side surface 614, and both of theobject-side surface 612 and the image-side surface 614 are aspheric. Theobject-side surface 612 has one inflection point.

The second lens element 620 has negative refractive power and it is madeof plastic material. The second lens element 620 has a convexobject-side surface 622 and a concave image-side surface 624, and bothof the object-side surface 622 and the image-side surface 624 areaspheric and have an inflection point.

The third lens element 630 has positive refractive power and it is madeof plastic material. The third lens element 630 has a convex object-sidesurface 632 and a concave image-side surface 634, and both of theobject-side surface 632 and the image-side surface 634 are aspheric andhave two inflection points.

The fourth lens element 640 has positive refractive power and it is madeof plastic material. The fourth lens element 640 has a concaveobject-side surface 642 and a convex image-side surface 644, and both ofthe object-side surface 642 and the image-side surface 644 are asphericand have one inflection point.

The fifth lens element 650 has positive refractive power and it is madeof plastic material. The fifth lens element 650 has a convex object-sidesurface 652 and a concave image-side surface 654, and both of theobject-side surface 652 and the image-side surface 654 are aspheric. Theobject-side surface 652 has two inflection points and the image-sidesurface 654 has four inflection points.

The sixth lens element 660 has negative refractive power and it is madeof plastic material. The sixth lens element 660 has a convex object-sidesurface 662 and a concave image-side surface 664. The object-sidesurface 662 has three inflection points and the image-side surface 664has one inflection point. Hereby, the back focal length is reduced tominiaturize the lens element effectively. In addition, the angle ofincident with incoming light from an off-axis view field can besuppressed effectively and the aberration in the off-axis view field canbe corrected further.

The IR-bandstop filter 680 is made of plastic material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 660 and the image plane 690.

In the optical image capturing system of the sixth embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relations are satisfied: ΣPP=30.900 mm andf1/ΣPP=0.308. Hereby, it is favorable for allocating the positiverefractive power of a single lens element to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the sixth embodiment, a sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relations are satisfied: ΣNP=−12.135 mm andf2/ΣNP=0.755. Hereby, it is favorable for allocating the negativerefractive power of a single lens element to other negative lenselements.

Please refer to the following Table 11 and Table 12.

The detailed data of the optical image capturing system of the sixthEmbodiment is as shown in Table 11.

TABLE 11 Data of the optical image capturing system f = 4.725 mm; f/HEP= 2.1; HAF = 40.000 deg Focal Surface # Curvature Radius ThicknessMaterial Index Abbe # length 0 Object Plano At infinity 1 Ape. stopPlano −0.049 2 Lens 1 6.418087091 0.672 Plastic 1.544 55.96 9.514 3−26.30906178 0.000 4 1E+18 0.275 5 Lens 2 5.848782949 0.350 Plastic1.642 22.46 −9.164 6 2.876462474 0.240 7 Lens 3 3.356045179 0.896Plastic 1.544 55.96 6.596 8 44.347765 0.703 9 Lens 4 −1.989874935 0.900Plastic 1.544 55.96 3.874 10 −1.189492013 0.050 11 Lens 5 3.0765727270.374 Plastic 1.642 22.46 10.916 12 5.186796264 0.119 13 Lens 611.61085018 0.525 Plastic 1.642 22.46 −2.971 14 1.621265352 0.658 15IR-bandstop Plano 0.420 BK_7 1.517 64.13 filter 16 Plano 1.180 17 Imageplane Plano 0.000 Reference wavelength (d-line) = 555 nmAs for the parameters of the aspheric surfaces of the sixth Embodiment,reference is made to Table 12.

TABLE 12 Aspheric Coefficients Surface # 2 3 5 6 7 8 9 k −3.577098E+00−8.999993E+01 4.563346E+00 −1.809963E+01 −2.490308E+01  −6.850519E+01 −7.466137E−01  A4 −1.614981E−02 −3.997416E−02 −7.208836E−02 −9.100254E−03 1.380851E−02 −1.981236E−02  4.183082E−03 A6  8.056891E−02 1.457079E−02 4.244343E−02  7.365986E−03 −1.679258E−02  5.712571E−037.835227E−03 A8 −4.653965E−01 −4.679363E−02 −6.121506E−02  −2.168610E−023.730947E−03 −4.260480E−03  −1.190465E−02  A10  1.204634E+00 4.733791E−02 4.888158E−02  1.763777E−02 2.299739E−03 1.643507E−031.075991E−02 A12 −1.739630E+00 −2.586364E−02 −2.446287E−02 −8.521531E−03 −2.760546E−03  −4.893522E−04  −4.502008E−03  A14 1.424545E+00  6.877498E−03 6.885859E−03  2.260578E−03 9.205001E−044.688325E−05 8.640735E−04 A16 −6.196196E−01 −6.474023E−04 −7.941251E−04 −2.434879E−04 −9.939355E−05  3.121277E−06 −6.118012E−05  A18 1.112092E−01  0.000000E+00 0.000000E+00  0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A20  0.000000E+00  0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 Surface # 10 11 1213 14 k −2.475324E+00 6.783026E−02 −3.036461E+00  −8.999813E+01 −4.697678E+00 A4 −5.101796E−02 −1.493594E−02  1.701641E−01 1.988599E−01−2.308567E−04 A6  2.157140E−02 −3.432182E−02  −1.905458E−01 −1.749846E−01  −8.463408E−03 A8 −1.218916E−02 1.983464E−02 8.377814E−026.648101E−02  2.891136E−03 A10  5.851308E−03 −5.176528E−03 −1.938203E−02  −1.354048E−02  −4.909239E−04 A12 −1.589657E−036.714175E−04 2.494756E−03 1.548485E−03  4.670323E−05 A14  2.234021E−04−4.404655E−05  −1.700367E−04  −9.409444E−05  −2.374731E−06 A16−1.220043E−05 1.280996E−06 4.805152E−06 2.368132E−06  4.999210E−08 A18 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00  0.000000E+00 A20 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00  0.000000E+00

In the sixth Embodiment, the presentation of the aspheric surfaceformula is similar to that in the first embodiment. Besides, thedefinitions of parameters in following tables are equal to those in thefirst embodiment, so the repetitious details will not be given here.

The following contents may be deduced from Table 11 and Table 12.

Sixth Embodiment (Primary reference wavelength: 555 nm) | f/f1 | | f/f2| | f/f3 | | f/f4 | | f/f5 | | f/f6 | 0.49664 0.51559 0.71638 1.219520.43282 1.59029 Σ PPR Σ NPR Σ PPR/| Σ NPR | IN12/f IN56/f TP4/(IN34 +TP4 + IN45) 2.86536 2.10588 1.36064 0.05816 0.02510 0.54448 | f1/f2 | |f2/f3 | (TP1 + IN12)/TP2 (TP6 + IN56)/TP5 1.03817 1.38942 2.703911.72292 HOS InTL HOS/HOI InS/HOS ODT % TDT % 7.36052 5.10292 1.840130.99328 1.30328 0.57440 HVT51 HVT52 HVT61 HVT62 HVT62/HOI HVT62/HOS1.76377 2.20518 2.65502 2.68582 0.67146 0.36490 TP2/TP3 TP3/TP4 InRS61InRS62 | InRS61 |/TP6 | InRS62 |/TP6 0.39051 0.99585 0.25112 0.523830.47798 0.99707 PLTA PSTA NLTA NSTA SLTA SSTA −0.019 mm −0.013 mm0.00034 mm −0.014 mm −0.006 mm −0.008 mm

The numerical related to the length of outline curve is shown accordingto table 11 and table 12.

Sixth embodiment (Reference wavelength = 555 nm) ARE ½(HEP) ARE valueARE − ½(HEP) 2(ARE/HEP) % TP ARE/TP (%) 11 1.125 1.126 0.00101 100.09%0.672 167.67% 12 1.125 1.133 0.00801 100.71% 0.672 168.71% 21 1.1251.125 0.00044 100.04% 0.350 321.54% 22 1.125 1.132 0.00747 100.66% 0.350323.55% 31 1.125 1.132 0.00743 100.66% 0.896 126.35% 32 1.125 1.124−0.00064 99.94% 0.896 125.45% 41 1.125 1.179 0.05377 104.78% 0.900130.97% 42 1.125 1.244 0.11880 110.56% 0.900 138.20% 51 1.125 1.1370.01201 101.07% 0.374 304.20% 52 1.125 1.140 0.01511 101.34% 0.374305.03% 61 1.125 1.137 0.01190 101.06% 0.525 216.39% 62 1.125 1.1650.04002 103.56% 0.525 221.75% ARS EHD ARS value ARS − EHD (ARS/EHD) % TPARS/TP (%) 11 1.134 1.135 0.001 100.10% 0.672 169.01% 12 1.334 1.3650.031 102.36% 0.672 203.27% 21 1.488 1.508 0.020 101.36% 0.350 430.98%22 1.715 1.730 0.016 100.92% 0.350 494.42% 31 1.836 1.848 0.013 100.69%0.896 206.21% 32 1.997 2.076 0.079 103.95% 0.896 231.64% 41 2.060 2.2610.201 109.76% 0.900 251.23% 42 2.151 2.569 0.418 119.42% 0.900 285.47%51 2.542 2.695 0.153 106.00% 0.374 721.02% 52 2.838 2.891 0.053 101.87%0.374 773.45% 61 2.992 3.025 0.034 101.13% 0.525 575.84% 62 3.391 3.5000.109 103.22% 0.525 666.17%

The following contents may be deduced from Table 11 and Table 12.

Related inflection point values of sixth embodiment (Primary referencewavelength: 555 nm) HIF111 0.7390 HIF111/HOI 0.1847 SGI111 0.0377|SGI111|/(|SGI111| + TP1) 0.0531 HIF211 0.5098 HIF211/HOI 0.1275 SGI2110.0181 |SGI211|/(|SGI211| + TP2) 0.0492 HIF221 0.7628 HIF221/HOI 0.1907SGI221 0.0782 |SGI221|/(|SGI221| + TP2) 0.1827 HIF311 0.8762 HIF311/HOI0.2190 SGI311 0.0893 |SGI311|/(|SGI311| + TP3) 0.0906 HIF321 0.3173HIF321/HOI 0.0793 SGI321 0.0009 |SGI321|/(|SGI321| + TP3) 0.0010 HIF3221.8784 HIF322/HOI 0.4696 SGI322 −0.2687 |SGI322|/(|SGI322| + TP3) 0.2307HIF411 1.7039 HIF411/HOI 0.4260 SGI411 −0.6689 |SGI411|/(|SGI411| + TP4)0.4264 HIF421 1.6077 HIF421/HOI 0.4019 SGI421 −0.9071|SGI421|/(|SGI421| + TP4) 0.5020 HIF511 0.8639 HIF511/HOI 0.2160 SGI5110.1064 |SGI511|/(|SGI511| + TP5) 0.2216 HIF512 2.4152 HIF512/HOI 0.6038SGI512 −0.0742 |SGI512|/(|SGI512| + TP5) 0.1656 HIF521 0.8626 HIF521/HOI0.2156 SGI521 0.1081 |SGI521|/(|SGI521| + TP5) 0.2244 HIF522 1.5814HIF522/HOI 0.3954 SGI522 0.2092 |SGI522|/(|SGI522| + TP5) 0.3589 HIF5231.9491 HIF523/HOI 0.4873 SGI523 0.2312 |SGI523|/(|SGI523| + TP5) 0.3822HIF524 2.7402 HIF524/HOI 0.6850 SGI524 0.1084 |SGI524|/(|SGI524| + TP5)0.2248 HIF611 0.9297 HIF611/HOI 0.2324 SGI611 0.0998|SGI611|/(|SGI611| + TP6) 0.1596 HIF612 1.6449 HIF612/HOI 0.4112 SGI6120.1910 |SGI612|/(|SGI612| + TP6) 0.2666 HIF613 2.2300 HIF613/HOI 0.5575SGI613 0.2432 |SGI613|/(|SGI613| + TP6) 0.3164 HIF621 1.0512 HIF621/HOI0.2628 SGI621 0.2542 |SGI621|/(|SGI621| + TP6) 0.3261

The Seventh Embodiment (Embodiment 7)

Please refer to FIG. 7A, FIG. 7B and FIG. 7C, FIG. 7A is a schematicview of the optical image capturing system according to the seventhEmbodiment of the present application, FIG. 7B is longitudinal sphericalaberration curves, astigmatic field curves, and an optical distortioncurve of the optical image capturing system in the order from left toright according to the seventh Embodiment of the present application,and FIG. 7C is a lateral aberration diagram of tangential fan, sagittalfan, the longest operation wavelength and the shortest operationwavelength passing through an edge of the entrance pupil and incident onthe image plane by 0.7 HOI according to the seventh embodiment of thepresent application. As shown in FIG. 7A, in order from an object sideto an image side, the optical image capturing system includes anaperture stop 700, a first lens element 710, a second lens element 720,a third lens element 730, a fourth lens element 740, a fifth lenselement 750, a sixth lens element 760, an IR-bandstop filter 780, animage plane 790, and an image sensing device 792.

The first lens element 710 has positive refractive power and it is madeof plastic material. The first lens element 710 has a convex object-sidesurface 712 and a concave image-side surface 714, and both of theobject-side surface 712 and the image-side surface 714 are aspheric andhave one inflection point.

The second lens element 720 has negative refractive power and it is madeof plastic material. The second lens element 720 has a convexobject-side surface 722 and a concave image-side surface 724, and bothof the object-side surface 722 and the image-side surface 724 areaspheric. The object-side surface 722 has one inflection point and theimage-side surface 724 has two inflection points.

The third lens element 730 has positive refractive power and it is madeof plastic material. The third lens element 730 has a convex object-sidesurface 732 and a convex image-side surface 734, and both of theobject-side surface 732 and the image-side surface 734 are aspheric. Theobject-side surface 732 has two inflection points and the image-sidesurface 734 has one inflection point.

The fourth lens element 740 has positive refractive power and it is madeof plastic material. The fourth lens element 740 has a concaveobject-side surface 742 and a convex image-side surface 744, and both ofthe object-side surface 742 and the image-side surface 744 are asphericand have one inflection point.

The fifth lens element 750 has positive refractive power and it is madeof plastic material. The fifth lens element 750 has a convex object-sidesurface 752 and a convex image-side surface 754, and both of theobject-side surface 752 and the image-side surface 754 are aspheric. Theobject-side surface 752 has two inflection points and the image-sidesurface 754 has three inflection points.

The sixth lens element 760 has negative refractive power and it is madeof plastic material. The sixth lens element 760 has a convex object-sidesurface 762 and a concave image-side surface 764. The object-sidesurface 762 has three inflection points and the image-side surface 764has one inflection point. Hereby, the back focal length is reduced tominiaturize the lens element effectively. In addition, the angle ofincident with incoming light from an off-axis view field can besuppressed effectively and the aberration in the off-axis view field canbe corrected further.

The IR-bandstop filter 780 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 760 and the image plane 790.

In the optical image capturing system of the seventh embodiment, a sumof focal lengths of all lens elements with positive refractive power isΣPP. The following relations are satisfied: ΣPP=28.122 mm andf1/ΣPP=0.365. Hereby, it is favorable for allocating the positiverefractive power of a single lens element to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the seventh embodiment, a sumof focal lengths of all lens elements with negative refractive power isΣNP. The following relations are satisfied: ΣNP=−13.355 mm andf2/ΣNP=0.807. Hereby, it is favorable for allocating the negativerefractive power of a single lens element to other negative lenselements.

Please refer to the following Table 13 and Table 14.

The detailed data of the optical image capturing system of the seventhEmbodiment is as shown in Table 13.

TABLE 13 Data of the optical image capturing system f = 4.711 mm; f/HEP= 2.2; HAF = 40 deg Focal Surface # Curvature Radius Thickness MaterialIndex Abbe # length 0 Object Plano At infinity 1 Ape. stop Plano −0.1222 Lens 1 3.689967156 0.619 Plastic 1.544 55.96 10.265 3 10.150516730.000 4 1E+18 0.308 5 Lens 2 4.932154633 0.400 Plastic 1.642 22.46−10.774 6 2.797467649 0.230 7 Lens 3 4.674874411 0.836 Plastic 1.54455.96 5.397 8 −7.478400266 0.548 9 Lens 4 −1.757075359 0.897 Plastic1.544 55.96 3.881 10 −1.134088735 0.050 11 Lens 5 96.86973929 0.561Plastic 1.642 22.46 8.580 12 −5.88113609 0.050 13 Lens 6 4.2315442820.467 Plastic 1.642 22.46 −2.581 14 1.146409695 0.643 15 IR-bandstopPlano 0.420 BK_7 1.517 64.13 filter 16 Plano 1.180 17 Image plane PlanoReference wavelength (d-line) = 555 nmAs for the parameters of the aspheric surfaces of the seventhEmbodiment, reference is made to Table 14.

TABLE 14 Aspheric Coefficients Surface # 2 3 5 6 7 8 9 k −3.379632E+01−8.998194E+01 −5.878008E+01 −2.463364E+01  −2.166010E+00 −6.851399E+01−7.582192E−01 A4  7.993994E−02 −4.047801E−02 −6.418745E−02 5.046145E−03−4.763981E−02 −6.132121E−02 −6.210813E−02 A6 −5.724971E−02  3.613439E−02 5.572651E−03 −7.469460E−02   3.941855E−02  3.915203E−02  9.760690E−02A8 −1.518440E−01 −8.313819E−02 −5.048433E−02 7.786042E−02 −4.772409E−02−3.104210E−02 −8.334447E−02 A10  6.856154E−01  9.463156E−02 8.171308E−02 −5.199731E−02   3.810534E−02  1.580021E−02  4.249573E−02A12 −1.223256E+00 −7.111641E−02 −7.435358E−02 1.885257E−02 −1.835547E−02−4.127622E−03 −1.239566E−02 A14  1.151111E+00  2.874412E−02 3.213441E−02 −3.477134E−03   4.368274E−03  4.437079E−04  1.996034E−03A16 −5.606967E−01 −5.027443E−03 −5.466707E−03 2.819103E−04 −3.816040E−04−4.593235E−06 −1.365572E−04 A18  1.112092E−01  0.000000E+00 0.000000E+00 0.000000E+00  0.000000E+00  0.000000E+00  0.000000E+00 A20 0.000000E+00  0.000000E+00  0.000000E+00 0.000000E+00  0.000000E+00 0.000000E+00  0.000000E+00 Surface # 10 11 12 13 14 k −2.583036E+001.682817E+01 1.415192E+00 −9.000000E+01 −4.843079E+00 A4 −5.368869E−021.436503E−02 −2.228284E−03  −3.286713E−02 −3.645622E−02 A6  4.590223E−021.381287E−02 3.719581E−02  1.913133E−02  1.312376E−02 A8 −3.498679E−02−1.496343E−02  −1.642807E−02  −4.962593E−03 −3.457824E−03 A10 1.456705E−02 5.747930E−03 3.361391E−03  7.714750E−04  5.793743E−04 A12−3.174696E−03 −1.291033E−03  −3.777368E−04  −7.708023E−05 −5.791376E−05A14  3.102134E−04 1.560978E−04 2.291097E−05  4.609233E−06  3.132798E−06A16 −5.824910E−06 −7.534341E−06  −5.923138E−07  −1.245570E−07−7.076410E−08 A18  0.000000E+00 0.000000E+00 0.000000E+00  0.000000E+00 0.000000E+00 A20  0.000000E+00 0.000000E+00 0.000000E+00  0.000000E+00 0.000000E+00

In the seventh Embodiment, the presentation of the aspheric surfaceformula is similar to that in the first embodiment. Besides, thedefinitions of parameters in following tables are equal to those in thefirst embodiment, so the repetitious details will not be given here.

The following contents may be deduced from Table 13 and Table 14.

The numerical related to the length of outline curve is shown accordingto table 13 and table 14.

Seventh embodiment (Reference wavelength = 555 nm) ARE ARE − 2(ARE/ ARE/ARE 1/2(HEP) value 1/2(HEP) HEP) % TP TP (%) 11 1.071 1.083 0.01209101.13% 0.619 174.78% 12 1.071 1.071 0.00087 100.08% 0.619 172.97% 211.071 1.075 0.00451 100.42% 0.400 268.78% 22 1.071 1.075 0.00417 100.39%0.400 268.70% 31 1.071 1.073 0.00279 100.26% 0.836 128.39% 32 1.0711.079 0.00819 100.77% 0.836 129.04% 41 1.071 1.143 0.07268 106.79% 0.897127.42% 42 1.071 1.174 0.10357 109.67% 0.897 130.86% 51 1.071 1.0710.00012 100.01% 0.561 190.94% 52 1.071 1.073 0.00202 100.19% 0.561191.28% 61 1.071 1.071 0.00087 100.08% 0.467 229.62% 62 1.071 1.1140.04350 104.06% 0.467 238.75% ARS ARS − (ARS/ ARS/ ARS EHD value EHDEHD) % TP TP (%) 11 1.097 1.109 0.013 101.14% 0.619 179.08% 12 1.2361.246 0.011 100.87% 0.619 201.21% 21 1.289 1.333 0.044 103.40% 0.400333.33% 22 1.554 1.576 0.022 101.42% 0.400 394.12% 31 1.699 1.711 0.012100.69% 0.836 204.69% 32 1.858 1.923 0.064 103.46% 0.836 229.96% 411.912 2.144 0.232 112.13% 0.897 238.96% 42 2.023 2.465 0.442 121.86%0.897 274.73% 51 2.343 2.442 0.098 104.20% 0.561 435.38% 52 2.742 2.7490.007 100.26% 0.561 490.28% 61 3.062 3.080 0.018 100.58% 0.467 660.02%62 3.428 3.577 0.149 104.34% 0.467 766.56%

The following contents may be deduced from Table 13 and Table 14.

Related inflection point values of seventh embodiment (Primary referencewavelength: 555 nm) HIF111 0.9928 HIF111/HOI 0.2482 SGI111 0.1284 |SGI111 |/(| SGI111 | + TP1) 0.1717 HIF121 0.4414 HIF121/HOI 0.1104SGI121 0.0079 | SGI121 |/(| SGI121 | + TP1) 0.0125 HIF211 0.3983HIF211/HOI 0.0996 SGI211 0.0132 | SGI211 |/(| SGI211 | + TP2) 0.0319HIF221 0.5880 HIF221/HOI 0.1470 SGI221 0.0493 | SGI221 |/(| SGI221 | +TP2) 0.1097 HIF222 1.5218 HIF222/HOI 0.3805 SGI222 −0.0092 | SGI222 |/(|SGI222 | + TP2) 0.0225 HIF311 0.7748 HIF311/HOI 0.1937 SGI311 0.0511 |SGI311 |/(| SGI311 | + TP3) 0.0576 HIF312 1.5850 HIF312/HOI 0.3963SGI312 0.0356 | SGI312 |/(| SGI312 | + TP3) 0.0409 HIF321 1.6678HIF321/HOI 0.4170 SGI321 −0.3363 | SGI321 |/(| SGI321 | + TP3) 0.2868HIF411 1.4043 HIF411/HOI 0.3511 SGI411 −0.5995 | SGI411 |/(| SGI411 | +TP4) 0.4005 HIF421 1.7416 HIF421/HOI 0.4354 SGI421 −1.0579 | SGI421 |/(|SGI421 | + TP4) 0.5411 HIF511 1.2156 HIF511/HOI 0.3039 SGI511 0.0415 |SGI511 |/(| SGI511 | + TP5) 0.0689 HIF512 2.2457 HIF512/HOI 0.5614SGI512 −0.2063 | SGI512 |/(| SGI512 | + TP5) 0.2689 HIF521 0.7224HIF521/HOI 0.1806 SGI521 −0.0412 | SGI521 |/(| SGI521 | + TP5) 0.0684HIF522 1.7310 HIF522/HOI 0.4328 SGI522 −0.0289 | SGI522 |/(| SGI522 | +TP5) 0.0491 HIF523 2.4396 HIF523/HOI 0.6099 SGI523 0.0176 | SGI523 |/(|SGI523 | + TP5) 0.0305 HIF611 0.5094 HIF611/HOI 0.1273 SGI611 0.0225 |SGI611 |/(| SGI611 | + TP6) 0.0460 HIF612 1.0747 HIF612/HOI 0.2687SGI612 0.0541 | SGI612 |/(| SGI612 | + TP6) 0.1039 HIF613 2.2590HIF613/HOI 0.5647 SGI613 0.1843 | SGI613 |/(| SGI613 | + TP6) 0.2832HIF621 0.8290 HIF621/HOI 0.2073 SGI621 0.2056 | SGI621 |/(| SGI621 | +TP6) 0.3058

The Eighth Embodiment (Embodiment 8)

Please refer to FIG. 8A, FIG. 8B and FIG. 8C, FIG. 8A is a schematicview of the optical image capturing system according to the eighthEmbodiment of the present application, FIG. 8B is longitudinal sphericalaberration curves, astigmatic field curves, and an optical distortioncurve of the optical image capturing system in the order from left toright according to the eighth Embodiment of the present application, andFIG. 8C is a lateral aberration diagram of tangential fan, sagittal fan,the longest operation wavelength and the shortest operation wavelengthpassing through an edge of the entrance pupil and incident on the imageplane by 0.7 HOI according to the eighth embodiment of the presentapplication. As shown in FIG. 8A, in order from an object side to animage side, the optical image capturing system includes an aperture stop800, a first lens element 810, a second lens element 820, a third lenselement 830, a fourth lens element 840, a fifth lens element 850, asixth lens element 860, an IR-bandstop filter 880, an image plane 890,and an image sensing device 892.

The first lens element 810 has positive refractive power and it is madeof plastic material. The first lens element 810 has a convex object-sidesurface 812 and a convex image-side surface 814, both of the object-sidesurface 812 and the image-side surface 814 are aspheric, and theobject-side surface 812 has one inflection point.

The second lens element 820 has negative refractive power and it is madeof plastic material. The second lens element 820 has a convexobject-side surface 822 and a concave image-side surface 824, and bothof the object-side surface 822 and the image-side surface 824 areaspheric and have one inflection point.

The third lens element 830 has positive refractive power and it is madeof plastic material. The third lens element 830 has a convex object-sidesurface 832 and a concave image-side surface 834, and both of theobject-side surface 832 and the image-side surface 834 are aspheric. Theobject-side surface 832 and the image-side surface 834 both have twoinflection points.

The fourth lens element 840 has positive refractive power and it is madeof plastic material. The fourth lens element 840 has a concaveobject-side surface 842 and a convex image-side surface 844, and both ofthe object-side surface 842 and the image-side surface 844 are asphericand have two inflection points.

The fifth lens element 850 has positive refractive power and it is madeof plastic material. The fifth lens element 850 has a convex object-sidesurface 852 and a convex image-side surface 854, and both of theobject-side surface 852 and the image-side surface 854 are aspheric. Theobject-side surface 852 has one inflection point and the image-sidesurface 854 has three inflection points.

The sixth lens element 860 has negative refractive power and it is madeof plastic material. The sixth lens element 860 has a convex object-sidesurface 862 and a concave image-side surface 864. The object-sidesurface 862 has three infection points and the image-side surface 864has an inflection point. Hereby, the back focal length is reduced tominiaturize the lens element effectively. In addition, the angle ofincident with incoming light from an off-axis view field can besuppressed effectively and the aberration in the off-axis view field canbe corrected further.

The IR-bandstop filter 880 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 860 and the image plane 890.

In the optical image capturing system of the eighth embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relations are satisfied: ΣPP=41.462 mm andf1/ΣPP=0.258. Hereby, it is favorable for allocating the positiverefractive power of a single lens element to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the sixth embodiment, a sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relations are satisfied: ΣNP=−11.880 mm andf2/ΣNP=0.718. Hereby, it is favorable for allocating the negativerefractive power of a single lens element to other negative lenselements.

Please refer to the following Table 15 and Table 16.

The detailed data of the optical image capturing system of the eighthEmbodiment is as shown in Table 15.

TABLE 15 Data of the optical image capturing system f = 5.692 mm; f/HEP= 2.4; HAF = 35 deg Focal Surface # Curvature Radius Thickness MaterialIndex Abbe # length 0 Object Plano At infinity 1 Ape. stop Plano −0.0462 Lens 1 6.44826438 0.590 Plastic 1.535 56.27 10.690 3 −50.048420970.000 4 1E+18 0.050 5 Lens 2 5.136996688 0.384 Plastic 1.642 22.46−8.525 6 2.582758219 0.230 7 Lens 3 2.688822867 0.872 Plastic 1.54455.96 5.697 8 17.50601916 1.402 9 Lens 4 −4.055690035 0.664 Plastic1.544 55.96 5.438 10 −1.820026986 0.050 11 Lens 5 26.61000897 0.719Plastic 1.636 23.89 19.637 12 −23.58433128 0.141 13 Lens 6 4.9937251260.491 Plastic 1.584 29.88 −3.355 14 1.36184563 0.508 15 IR-bandstopPlano 0.420 BK_7 1.517 64.13 filter 16 Plano 1.080 17 Image plane Plano0.000 Reference wavelength (d-line) = 555 nmAs for the parameters of the aspheric surfaces of the eighth Embodiment,reference is made to Table 16.

TABLE 16 Aspheric Coefficients Surface # 2 3 5 6 7 8 9 k −5.333361E+01 −8.999999E+01  −5.473051E+01 −1.901772E+01  −6.066082E+00 −6.826703E+01−5.026658E+00 A4 2.168529E−03 1.612771E−02  4.177854E−02 3.863449E−02−2.745188E−02 −7.361940E−03 −4.979395E−03 A6 4.549983E−02 −1.198037E−01 −1.076120E−01 −6.753276E−02   2.210781E−02 −1.567062E−03  3.874409E−02A8 −2.518198E−01  1.284617E−01  1.129303E−01 6.939839E−02 −2.266745E−02−4.446754E−03 −3.103542E−02 A10 5.381608E−01 −8.039838E−02 −6.657323E−02 −4.344836E−02   1.757183E−02  3.524714E−03  1.449552E−02A12 −6.542111E−01  2.741260E−02  1.868909E−02 1.419273E−02 −8.443962E−03−1.268843E−03 −4.173296E−03 A14 4.604013E−01 −4.303709E−03 −1.243411E−03 −2.123967E−03   2.079436E−03  2.009075E−04  6.543242E−04A16 −1.745914E−01  1.530499E−04 −2.744826E−04 9.141563E−05 −1.976974E−04−8.571534E−06 −4.322824E−05 A18 2.758492E−02 0.000000E+00  0.000000E+000.000000E+00  0.000000E+00  0.000000E+00  0.000000E+00 A20 0.000000E+000.000000E+00  0.000000E+00 0.000000E+00  0.000000E+00  0.000000E+00 0.000000E+00 Surface # 10 11 12 13 14 k −4.240850E+00 7.228888E+016.982490E+01 −8.999981E+01 −5.585469E+00 A4 −1.048717E−02 4.480112E−028.914610E−02 −1.349158E−02 −4.893631E−02 A6  3.060725E−02 −3.279198E−02 −8.498529E−02  −3.541200E−02  1.511882E−02 A8 −2.141839E−02 6.167751E−033.623295E−02  1.984972E−02 −2.670990E−03 A10  9.780697E−03 1.239302E−03−9.153587E−03  −4.566674E−03  2.834819E−04 A12 −2.704849E−03−1.023917E−03  1.378247E−03  5.499138E−04 −1.794875E−05 A14 3.902002E−04 1.975407E−04 −1.129991E−04  −3.438804E−05  6.161371E−07A16 −2.260285E−05 −1.228442E−05  3.867899E−06  8.837712E−07−8.806711E−09 A18  0.000000E+00 0.000000E+00 0.000000E+00  0.000000E+00 0.000000E+00 A20  0.000000E+00 0.000000E+00 0.000000E+00  0.000000E+00 0.000000E+00

In the eighth Embodiment, the presentation of the aspheric surfaceformula is similar to that in the first embodiment. Besides, thedefinitions of parameters in following tables are equal to those in thefirst embodiment, so the repetitious details will not be given here.

The following contents may be deduced from Table 15 and Table 16.

Eighth Embodiment (Primary reference wavelength: 555 nm) | f/f1 | | f/f2| | f/f3 | | f/f4 | | f/f5 | | f/f6 | 0.53249 0.66770 0.99916 1.046640.28987 1.69644 Σ PPR Σ ENPR Σ PPR/| Σ NPR | IN12/f IN56/f TP4/(IN34 +TP4 + IN45) 2.86815 2.36414 1.21319 0.00878 0.02471 0.31362 | f1/f2 | |f2/f3 | (TP1 + IN12)/TP2 (TP6 + IN56)/TP5 1.25392 1.49642 1.664840.87817 HOS InTL HOS/HOI InS/HOS ODT % TDT % 7.60000 5.59224 1.900000.99389  0.510618  0.303379 HVT51 HVT52 HVT61 HVT62 HVT62/HOI HVT62/HOS1.32617 0     0.86201 2.66679 0.66670 0.35089 TP2/TP3 TP3/TP4 InRS61InRS62 | InRS61 |/TP6 | InRS62 |/TP6 0.44117 1.31318 −0.21530  0.359070.43892 0.73201 PLTA PSTA NLTA NSTA SLTA SSTA −0.010 mm 0.002 mm 0.006mm 0.002 mm 0.001 mm −0.001 mm

The numerical related to the length of outline curve is shown accordingto table 15 and table 16.

Eighth embodiment (Primary reference wavelength = 555 nm) ARE ARE −2(ARE/ ARE/ ARE 1/2(HEP) value 1/2(HEP) HEP) % TP TP (%) 11 1.186 1.1870.00102 100.09% 0.590 201.12% 12 1.186 1.193 0.00673 100.57% 0.590202.09% 21 1.186 1.188 0.00217 100.18% 0.384 308.98% 22 1.186 1.2010.01501 101.27% 0.384 312.32% 31 1.186 1.202 0.01649 101.39% 0.872137.96% 32 1.186 1.185 −0.00065 99.95% 0.872 135.99% 41 1.186 1.1930.00762 100.64% 0.664 179.83% 42 1.186 1.226 0.03973 103.35% 0.664184.66% 51 1.186 1.186 0.00060 100.05% 0.719 165.08% 52 1.186 1.185−0.00069 99.94% 0.719 164.90% 61 1.186 1.187 0.00094 100.08% 0.491241.95% 62 1.186 1.218 0.03249 102.74% 0.491 248.38% ARS ARS − (ARS/ARS/ ARS EHD value EHD EHD) % TP TP (%) 11 1.194 1.196 0.001 100.12%0.590 202.65% 12 1.358 1.378 0.020 101.50% 0.590 233.56% 21 1.465 1.4680.003 100.21% 0.384 381.79% 22 1.634 1.653 0.019 101.13% 0.384 429.91%31 1.763 1.789 0.026 101.49% 0.872 205.31% 32 1.852 1.867 0.015 100.82%0.872 214.26% 41 2.032 2.083 0.050 102.48% 0.664 313.83% 42 2.193 2.2940.101 104.60% 0.664 345.58% 51 2.236 2.452 0.216 109.67% 0.719 341.16%52 2.675 2.767 0.092 103.46% 0.719 385.01% 61 2.969 2.995 0.026 100.89%0.491 610.60% 62 3.508 3.596 0.088 102.51% 0.491 733.06%

The following contents may be deduced from Table 15 and Table 16.

Related inflection point values of eighth Embodiment (Primary referencewavelength: 555 nm) HIF111 0.7240 H1F111/HOI 0.1810 SGI111 0.0355 |SGI111 |/(| SGI111 | + TP1) 0.0567 HIF211 0.7082 HIF211/HOI 0.1770SGI211 0.0426 | SGI211 |/(| SGI211 | + TP2) 0.0997 HIF221 0.9711HIF221/HOI 0.2428 SGI221 0.1355 | SGI221 |/(| SGI221 | + TP2) 0.2605HIF311 1.0618 HIF311/HOI 0.2655 SGI311 0.1585 | SGI311 |/(| SGI311 | +TP3) 0.1539 HIF312 1.6017 HIF312/HOI 0.4004 SGI312 0.2630 | SGI312 |/(|SGI312 | + TP3) 0.2318 HIF321 0.6249 HIF321/HOI 0.1562 SGI321 0.0096 |SGI321 |/(| SGI321 | + TP3) 0.0109 HIF322 1.7587 HIF322/HOI 0.4397SGI322 −0.0877 | SGI322 |/(| SGI322 | + TP3) 0.0914 HIF411 0.8932HIF411/HOI 0.2233 SGI411 −0.0863 | SGI411 |/(| SGI411 | + TP4) 0.1151HIF412 1.4419 HIF412/HOI 0.3605 SGI412 −0.1624 | SGI412 |/(| SGI412 | +TP4) 0.1966 HIF421 1.0205 HIF421/HOI 0.2551 SGI421 −0.2293 | SGI421 |/(|SGI421 | + TP4) 0.2568 HIF422 1.6740 HIF422/HOI 0.4185 SGI422 −0.4304 |SGI422 |/(| SGI422 | + TP4) 0.3934 HIF511 0.9396 HIF511/HOI 0.2349SGI511 0.0333 | SGI511 |/(| SGI511 | + TP5) 0.0443 HIF521 0.2110HIF521/HOI 0.0528 SGI521 −0.0008 | SGI521 |/(| SGI521 | + TP5) 0.0011HIF522 0.8056 HIF522/HOI 0.2014 SGI522 0.0057 | SGI522 |/(| SGI522 | +TP5) 0.0079 HIF523 2.5130 HIF523/HOI 0.6282 SGI523 −0.4033 | SGI523 |/(|SGI523 | + TP5) 0.3595 HIF611 0.4802 HIF611/HOI 0.1201 SGI611 0.0186 |SGI611 |/(| SGI611 | + TP6) 0.0364 HIF612 1.6007 HIF612/HOI 0.4002SG1612 −0.0781 | SGI612 |/(| SGI612 | + TP6) 0.1374 HIF613 2.4821HIF613/HOI 0.6205 SGI613 −0.1960 | SGI613 |/(| SGI613 | + TP6) 0.2854HIF621 0.7341 HIF621/HOI 0.1835 SGI621 0.1445 | SGI621 |/(| SGI621 | +TP6) 0.2276

The above-mentioned descriptions represent merely the exemplaryembodiment of the present disclosure, without any intention to limit thescope of the present disclosure thereto. Various equivalent changes,alternations or modifications based on the claims of present disclosureare all consequently viewed as being embraced by the scope of thepresent disclosure.

What is claimed is:
 1. An optical image capturing system, from an objectside to an image side, comprising: a first lens element with refractivepower; a second lens element with refractive power; a third lens elementwith refractive power; a fourth lens element with refractive power; afifth lens element with refractive power; a sixth lens element withrefractive power; and an image plane; wherein the optical imagecapturing system consists of the six lens elements with refractivepower, a maximum height for image formation on the image planeperpendicular to the optical axis in the optical image capturing systemis denoted by HOI, at least one of the first through sixth lens elementshas positive refractive power, focal lengths of the first through sixthlens elements are f1, f2, f3, f4, f5 and f6 respectively, a focal lengthof the optical image capturing system is f, an entrance pupil diameterof the optical image capturing system is HEP, a distance on an opticalaxis from an object-side surface of the first lens element to the imageplane is HOS, a distance on an optical axis from the object-side surfaceof the first lens element to the image-side surface of the sixth lenselement is InTL, a half of a maximum view angle of the optical imagecapturing system is HAF, a length of outline curve from an axial pointon any surface of any one of the six lens elements to a coordinate pointof vertical height with a distance of a half of the entrance pupildiameter from the optical axis on the surface along an outline of thesurface is denoted as ARE. The following relations are satisfied:1.0≦f/HEP≦10.0, 0 deg<HAF≦150 deg and 0.9≦2(ARE/HEP)≦1.5.
 2. The opticalimage capturing system of claim 1, wherein TV distortion for imageformation in the optical image capturing system is TDT, a maximum heightfor image formation on the image plane perpendicular to the optical axisin the optical image capturing system is denoted by HOI, a lateralaberration of the longest operation wavelength of a visible light of apositive direction tangential fan of the optical image capturing systempassing through an edge of the entrance pupil and incident on the imageplane by 0.7 HOI is denoted as PLTA, and a lateral aberration of theshortest operation wavelength of a visible light of the positivedirection tangential fan of the optical image capturing system passingthrough the edge of the entrance pupil and incident on the image planeby 0.7 HOI is denoted as PSTA, a lateral aberration of the longestoperation wavelength of a visible light of a negative directiontangential fan of the optical image capturing system passing through theedge of the entrance pupil and incident on the image plane by 0.7 HOT isdenoted as NLTA, a lateral aberration of the shortest operationwavelength of a visible light of a negative direction tangential fan ofthe optical image capturing system passing through the edge of theentrance pupil and incident on the image plane by 0.7 HOI is denoted asNSTA, a lateral aberration of the longest operation wavelength of avisible light of a sagittal fan of the optical image capturing systempassing through the edge of the entrance pupil and incident on the imageplane by 0.7 HOI is denoted as SLTA, a lateral aberration of theshortest operation wavelength of a visible light of the sagittal fan ofthe optical image capturing system passing through the edge of theentrance pupil and incident on the image plane by 0.7 HOI is denoted asSSTA. The following relations are satisfied: PLTA≦100 μm; PSTA≦100 μm;NLTA≦100 μm; NSTA≦100 μm; SLTA≦100 μm; and SSTA≦100 μm; |TDT|≦250%. 3.The optical image capturing system of claim 1, wherein a maximumeffective half diameter position of any surface of any one of the sixlens elements is denoted as EHD, and a length of outline curve from anaxial point on any surface of any one of the six lens elements to themaximum effective half diameter position of the surface along theoutline of the surface is denoted as ARS. The following relation issatisfied: 0.9≦ARS/EHD≦2.0.
 4. The optical image capturing system ofclaim 1, wherein the following relation is satisfied: 0 mm<HOS≦30 mm. 5.The optical image capturing system of claim 1, wherein a half of a viewangle of the optical image capturing system is HAF, and the followingrelation is satisfied: 0 deg<HAF≦100 deg.
 6. The optical image capturingsystem of claim 1, wherein a length of outline curve from an axial pointon the object-side surface of the sixth lens element to a coordinatepoint of vertical height with a distance of a half of the entrance pupildiameter from the optical axis on the surface along an outline of thesurface is denoted as ARE61; a length of outline curve from an axialpoint on the image-side surface of the sixth lens element to thecoordinate point of vertical height with the distance of a half of theentrance pupil diameter from the optical axis on the surface along theoutline of the surface is denoted as ARE62, and a thickness of the sixthlens element on the optical axis is TP6. The following relations aresatisfied: 0.05≦ARE61/TP6≦15, and 0.05≦ARE62/TP6≦15.
 7. The opticalimage capturing system of claim 1, wherein a length of outline curvefrom an axial point on the object-side surface of the fifth lens elementto a coordinate point of vertical height with a distance of a half ofthe entrance pupil diameter from the optical axis on the surface alongan outline of the surface is denoted as ARE51; a length of outline curvefrom an axial point on the image-side surface of the fifth lens elementto the coordinate point of vertical height with the distance of a halfof the entrance pupil diameter from the optical axis on the surfacealong the outline of the surface is denoted as ARE52, and a thickness ofthe fifth lens element on the optical axis is TP5. The followingrelations are satisfied: 0.05≦ARE51/TP5≦15; and 0.05≦ARE52/TP5≦15. 8.The optical image capturing system of claim 1, wherein at least one lenselement among the first through third lens elements has positiverefractive power.
 9. The optical image capturing system of claim 1,further comprising an aperture stop, a distance from the aperture stopto the image plane on the optical axis is InS, and the followingrelation is satisfied: 0.2≦InS/HOS≦1.1.
 10. An optical image capturingsystem, from an object side to an image side, comprising: a first lenselement with refractive power; a second lens element with refractivepower; a third lens element with refractive power; a fourth lens elementwith refractive power; a fifth lens element with refractive power; asixth lens element with refractive power; and an image plane; whereinthe optical image capturing system consists of the six lens elementswith refractive power, a maximum height for image formation on the imageplane perpendicular to the optical axis in the optical image capturingsystem is denoted by HOI, at least one lens element among the firstthrough sixth lens elements has at least one inflection point on atleast one surface thereof, at least one lens element among the firstthrough third lens elements has positive refractive power, at least onelens element among the fourth through sixth lens elements has positiverefractive power, focal lengths of the first through sixth lens elementsare f1, f2, f3, f4, f5 and f6 respectively, a focal length of theoptical image capturing system is f, an entrance pupil diameter of theoptical image capturing system is HEP, a distance on an optical axisfrom an object-side surface of the first lens element to the image planeis HOS, a distance on an optical axis from the object-side surface ofthe first lens element to the image-side surface of the sixth lenselement is InTL, a half of a maximum view angle of the optical imagecapturing system is HAF, a length of outline curve from an axial pointon any surface of any one of the six lens elements to a coordinate pointof vertical height with a distance of a half of the entrance pupildiameter from the optical axis on the surface along an outline of thesurface is denoted as ARE. The following relations are satisfied:1.0≦f/HEP≦10.0, 0 deg<HAF≦150 deg and 0.9≦2(ARE/HEP)≦1.5.
 11. Theoptical image capturing system of claim 10, wherein a maximum effectivehalf diameter position of any surface of any one of the six lenselements is denoted as EHD, and a length of outline curve from an axialpoint on any surface of any one of the six lens elements to the maximumeffective half diameter position of the surface along the outline of thesurface is denoted as ARS. The following relation is satisfied:0.9≧ARS/EHD≦2.0.
 12. The optical image capturing system of claim 10,wherein at least two lens elements among the first through sixth lenselements respectively has at least one inflection point on at least onesurface thereof.
 13. The optical image capturing system of claim 10,wherein a maximum height for image formation on the image planeperpendicular to the optical axis in the optical image capturing systemis denoted by HOI, a lateral aberration of the longest operationwavelength of a visible light of a positive direction tangential fan ofthe optical image capturing system passing through an edge of theentrance pupil and incident on the image plane by 0.7 HOI is denoted asPLTA, and a lateral aberration of the shortest operation wavelength of avisible light of the positive direction tangential fan of the opticalimage capturing system passing through the edge of the entrance pupiland incident on the image plane by 0.7 HOI is denoted as PSTA, a lateralaberration of the longest operation wavelength of a visible light of anegative direction tangential fan of the optical image capturing systempassing through the edge of the entrance pupil and incident on the imageplane by 0.7 HOT is denoted as NLTA, a lateral aberration of theshortest operation wavelength of a visible light of a negative directiontangential fan of the optical image capturing system passing through theedge of the entrance pupil and incident on the image plane by 0.7 HOI isdenoted as NSTA, a lateral aberration of the longest operationwavelength of a visible light of a sagittal fan of the optical imagecapturing system passing through the edge of the entrance pupil andincident on the image plane by 0.7 HOI is denoted as SLTA, a lateralaberration of the shortest operation wavelength of a visible light ofthe sagittal fan of the optical image capturing system passing throughthe edge of the entrance pupil and incident on the image plane by 0.7HOI is denoted as SSTA. The following relations are satisfied: PLTA≦100μm; PSTA≦100 μm; NLTA≦100 μm; NSTA≦100 μm; SLTA≦100 μm; SSTA≦100 μm andHOI>3.0 mm.
 14. The optical image capturing system of claim 10, whereinat least one of the first, the second, the third, the fourth, the fifthand the sixth lens elements is a light filtration element with awavelength of less than 500 nm.
 15. The optical image capturing systemof claim 10, wherein a distance between the first lens element and thesecond lens element on the optical axis is IN12, and the followingrelation is satisfied: 0<IN12/f≦3.0.
 16. The optical image capturingsystem of claim 10, wherein a distance between the fifth lens elementand the sixth lens element on the optical axis is IN56, and thefollowing relation is satisfied: 0<IN56/f≦0.8.
 17. The optical imagecapturing system of claim 10, wherein the distance from the fifth lenselement to the sixth lens element on the optical axis is IN56, athickness of the fifth lens element and a thickness of the sixth lenselement on the optical axis respectively are TP5 and TP6, and thefollowing relation is satisfied: 0.1≦(TP6+IN56)/TP5≦10.
 18. The opticalimage capturing system of claim 10, wherein the distance from the firstlens element to the second lens element on the optical axis is IN12, athickness of the first lens element and a thickness of the second lenselement on the optical axis respectively are TP1 and TP2, and thefollowing relation is satisfied: 0.1≦(TP1+IN12)/TP2≦10.
 19. The opticalimage capturing system of claim 10, wherein a thickness of the fourthlens element on the optical axis is TP4, a thickness of the fifth lenselement on the optical axis is TP5, a thickness of the sixth lenselement on the optical axis is TP6, and the following relation issatisfied: TP4≦TP5 and TP4≦TP6.
 20. An optical image capturing system,from an object side to an image side, comprising: a first lens elementwith positive refractive power; a second lens element with refractivepower; a third lens element with refractive power; a fourth lens elementwith refractive power; a fifth lens element with refractive power; asixth lens element with refractive power; and an image plane; whereinthe optical image capturing system consists of the six lens elementswith refractive power, a maximum height for image formation on the imageplane perpendicular to the optical axis in the optical image capturingsystem is denoted by HOI, at least one lens element among the secondthrough sixth lens elements has positive refractive power, at least twolens elements among the first through sixth lens elements respectivelyhave at least one inflection point on at least one surface thereof,focal lengths of the first through sixth lens elements are f1, f2, f3,f4, f5 and f6 respectively, a focal length of the optical imagecapturing system is f, an entrance pupil diameter of the optical imagecapturing system is HEP, a distance on an optical axis from anobject-side surface of the first lens element to the image plane is HOS,a distance on an optical axis from the object-side surface of the firstlens element to the image-side surface of the sixth lens element isInTL, a half of maximum view angle of the optical image capturing systemis HAF, a length of outline curve from an axial point on any surface ofany one of the six lens elements to a coordinate point of verticalheight with a distance of a half of the entrance pupil diameter from theoptical axis on the surface along an outline of the surface is denotedas ARE. The following relations are satisfied: 1.0≦f/HEP≦3.5, 0deg<HAF≦150 deg and 0.9≦2(ARE/HEP)≦1.5.
 21. The optical image capturingsystem of claim 20, wherein a maximum effective half diameter positionof any surface of any one of the six lens elements is denoted as EHD,and a length of outline curve from an axial point on any surface of anyone of the six lens elements to the maximum effective half diameterposition of the surface along the outline of the surface is denoted asARS. The following relation is satisfied: 0.9≦ARS/EHD≦2.0.
 22. Theoptical image capturing system of claim 20, wherein the followingrelation is satisfied: 0 mm<HOS≦30 mm.
 23. The optical image capturingsystem of claim 20, wherein a length of outline curve from an axialpoint on the object-side surface of the sixth lens element to acoordinate point of vertical height with a distance of a half of theentrance pupil diameter from the optical axis on the surface along anoutline of the surface is denoted as ARE61; a length of outline curvefrom an axial point on the image-side surface of the sixth lens elementto the coordinate point of vertical height with the distance of a halfof the entrance pupil diameter from the optical axis on the surfacealong the outline of the surface is denoted as ARE62, and a thickness ofthe sixth lens element on the optical axis is TP6. The followingrelations are satisfied: 0.05≦ARE61/TP6≦15 and 0.05≦ARE62/TP6≦15. 24.The optical image capturing system of claim 20, wherein a length ofoutline curve from an axial point on the object-side surface of thefifth lens element to a coordinate point of vertical height with adistance of a half of the entrance pupil diameter from the optical axison the surface along an outline of the surface is denoted as ARE51; alength of outline curve from an axial point on the image-side surface ofthe fifth lens element to the coordinate point of vertical height withthe distance of a half of the entrance pupil diameter from the opticalaxis on the surface along the outline of the surface is denoted asARE52, and a thickness of the fifth lens element on the optical axis isTP5. The following relations are satisfied: 0.05≦ARE51/TP5≦15 and0.05≦ARE52/TP5≦15.
 25. The optical image capturing system of claim 20,wherein the optical image capturing system further comprise an aperturestop, an image sensing device and a driving module, the image sensingdevice is disposed on the image plane, a distance from the aperture stopto the image plane is InS, and the driving module couples with the lenselements to displace the lens elements. The following relation issatisfied: 0.2≦InS/HOS≦1.1.